Optical image capturing system

ABSTRACT

An optical image capturing system includes, along the optical axis in order from an object side to an image side, a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. At least one lens among the first to the sixth lenses has positive refractive power. The seventh lens has negative refractive power, wherein both surfaces thereof are aspheric, and at least one surface thereof has an inflection point. The lenses in the optical image capturing system which have refractive power include the first to the seventh lenses. The optical image capturing system can increase aperture value and improve the imaging quality for use in compact cameras.

BACKGROUND OF THE INVENTION 1. Technical Field

The present invention relates generally to an optical system, and more particularly to a compact optical image capturing system for an electronic device.

2. Description of Related Art

In recent years, with the rise of portable electronic devices having camera functionalities, the demand for an optical image capturing system is raised gradually. The image sensing device of the ordinary photographing camera is commonly selected from charge coupled device (CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor). In addition, as advanced semiconductor manufacturing technology enables the minimization of the pixel size of the image sensing device, the development of the optical image capturing system towards the field of high pixels. Therefore, the requirement for high imaging quality is rapidly raised.

The conventional optical system of the portable electronic device usually has five or six lenses. However, the optical system is asked to take pictures in a dark environment, in other words, the optical system is asked to have a large aperture. The conventional optical system provides high optical performance as required.

It is an important issue to increase the quantity of light entering the lens. In addition, the modern lens is also asked to have several characters, including high image quality.

BRIEF SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an optical image capturing system and an optical image capturing lens which use combination of refractive powers, convex and concave surfaces of seven-piece optical lenses (the convex or concave surface in the disclosure denotes the geometrical shape of an image-side surface or an object-side surface of each lens on an optical axis) to increase the quantity of incoming light of the optical image capturing system, and to improve imaging quality for image formation, so as to be applied to minimized electronic products.

The term and its definition to the lens parameter in the embodiment of the present are shown as below for further reference.

The lens parameter related to a length or a height in the lens:

For visible spectrum, the present invention may adopt the wavelength of 555 nm as the primary reference wavelength and the basis for the measurement of focus shift; for infrared spectrum (700-1300 nm), the present invention may adopt the wavelength of 940 nm as the primary reference wavelength and the basis for the measurement of focus shift.

The optical image capturing system includes an image plane specifically for the infrared light which is perpendicular to the optical axis, wherein the through-focus modulation transfer rate (value of MTF) at a first spatial frequency has a maximum value in the central of field of view of the image plane specifically for the infrared light, wherein the first spatial frequency is denoted by SP1, which satisfies the following condition: SP1≤440 cycles/mm Preferably, the first spatial frequency satisfies the following condition: SP1≤220 cycles/mm.

A maximum height for image formation of the optical image capturing system is denoted by HOI. A height of the optical image capturing system is denoted by HOS. A distance from the object-side surface of the first lens to the image-side surface of the seventh lens is denoted by InTL. A distance between the aperture and the image plane specifically for the infrared light is denoted by InS. A distance from the first lens to the second lens is denoted by IN12 (instance). A central thickness of the first lens of the optical image capturing system on the optical axis is denoted by TP1 (instance).

The lens parameter related to a material in the lens:

An Abbe number of the first lens in the optical image capturing system is denoted by NA1 (instance). A refractive index of the first lens is denoted by Nd1 (instance).

The lens parameter related to a view angle in the lens:

A view angle is denoted by AF. Half of the view angle is denoted by HAF. A major light angle is denoted by MRA.

The lens parameter related to exit/entrance pupil in the lens:

An entrance pupil diameter of the optical image capturing system is denoted by HEP. An exit pupil diameter of the image-side surface of the seventh lens is denoted by HXP. For any surface of any lens, a maximum effective half diameter (EHD) is a perpendicular distance between an optical axis and a crossing point on the surface where the incident light with a maximum viewing angle of the system passing the very edge of the entrance pupil. For example, the maximum effective half diameter of the object-side surface of the first lens is denoted by EHD11, the maximum effective half diameter of the image-side surface of the first lens is denoted by EHD12, the maximum effective half diameter of the object-side surface of the second lens is denoted by EHD21, the maximum effective half diameter of the image-side surface of the second lens is denoted by EHD22, and so on.

The lens parameter related to an arc length of the shape of a surface and a surface profile:

For any surface of any lens, a profile curve length of the maximum effective half diameter is, by definition, measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to an end point of the maximum effective half diameter thereof. In other words, the curve length between the aforementioned start and end points is the profile curve length of the maximum effective half diameter, which is denoted by ARS. For example, the profile curve length of the maximum effective half diameter of the object-side surface of the first lens is denoted by ARS11, the profile curve length of the maximum effective half diameter of the image-side surface of the first lens is denoted by ARS12, the profile curve length of the maximum effective half diameter of the object-side surface of the second lens is denoted by ARS21, the profile curve length of the maximum effective half diameter of the image-side surface of the second lens is denoted by ARS22, and so on.

For any surface of any lens, a profile curve length of a half of the entrance pupil diameter (HEP) is, by definition, measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis. In other words, the curve length between the aforementioned stat point and the coordinate point is the profile curve length of a half of the entrance pupil diameter (HEP), and is denoted by ARE. For example, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the first lens is denoted by ARE11, the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens is denoted by ARE12, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the second lens is denoted by ARE21, the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens is denoted by ARE22, and so on.

The lens parameter related to a depth of the lens shape:

A displacement from a point on the object-side surface of the seventh lens, which is passed through by the optical axis, to a point on the optical axis, where a projection of the maximum effective semi diameter of the object-side surface of the seventh lens ends, is denoted by InRS71 (the depth of the maximum effective semi diameter). A displacement from a point on the image-side surface of the seventh lens, which is passed through by the optical axis, to a point on the optical axis, where a projection of the maximum effective semi diameter of the image-side surface of the seventh lens ends, is denoted by InRS72 (the depth of the maximum effective semi diameter). The depth of the maximum effective semi diameter (sinkage) on the object-side surface or the image-side surface of any other lens is denoted in the same manner

The lens parameter related to the lens shape:

A critical point C is a tangent point on a surface of a specific lens, and the tangent point is tangent to a plane perpendicular to the optical axis and the tangent point cannot be a crossover point on the optical axis. Following the above description, a distance perpendicular to the optical axis between a critical point C51 on the object-side surface of the fifth lens and the optical axis is HVT51 (instance), and a distance perpendicular to the optical axis between a critical point C52 on the image-side surface of the fifth lens and the optical axis is HVT52 (instance). A distance perpendicular to the optical axis between a critical point C61 on the object-side surface of the sixth lens and the optical axis is HVT61 (instance), and a distance perpendicular to the optical axis between a critical point C62 on the image-side surface of the sixth lens and the optical axis is HVT62 (instance). A distance perpendicular to the optical axis between a critical point on the object-side or image-side surface of other lenses, such as the seventh lens, and the optical axis is denoted in the same manner.

The object-side surface of the seventh lens has one inflection point IF711 which is nearest to the optical axis, and the sinkage value of the inflection point IF711 is denoted by SGI711 (instance). A distance perpendicular to the optical axis between the inflection point IF711 and the optical axis is HIF711 (instance). The image-side surface of the seventh lens has one inflection point IF721 which is nearest to the optical axis, and the sinkage value of the inflection point IF721 is denoted by SGI721 (instance). A distance perpendicular to the optical axis between the inflection point IF721 and the optical axis is HlF721 (instance).

The object-side surface of the seventh lens has one inflection point IF712 which is the second nearest to the optical axis, and the sinkage value of the inflection point IF712 is denoted by SGI712 (instance). A distance perpendicular to the optical axis between the inflection point IF712 and the optical axis is HIF712 (instance). The image-side surface of the seventh lens has one inflection point IF722 which is the second nearest to the optical axis, and the sinkage value of the inflection point IF722 is denoted by SGI722 (instance). A distance perpendicular to the optical axis between the inflection point IF722 and the optical axis is HIF722 (instance).

The object-side surface of the seventh lens has one inflection point IF713 which is the third nearest to the optical axis, and the sinkage value of the inflection point IF713 is denoted by SGI713 (instance). A distance perpendicular to the optical axis between the inflection point IF713 and the optical axis is HIF713 (instance). The image-side surface of the seventh lens has one inflection point IF723 which is the third nearest to the optical axis, and the sinkage value of the inflection point IF723 is denoted by SGI723 (instance). A distance perpendicular to the optical axis between the inflection point IF723 and the optical axis is HIF723 (instance).

The object-side surface of the seventh lens has one inflection point IF714 which is the fourth nearest to the optical axis, and the sinkage value of the inflection point IF714 is denoted by SGI714 (instance). A distance perpendicular to the optical axis between the inflection point IF714 and the optical axis is HIF714 (instance). The image-side surface of the seventh lens has one inflection point IF724 which is the fourth nearest to the optical axis, and the sinkage value of the inflection point IF724 is denoted by SGI724 (instance). A distance perpendicular to the optical axis between the inflection point IF724 and the optical axis is HIF724 (instance).

An inflection point, a distance perpendicular to the optical axis between the inflection point and the optical axis, and a sinkage value thereof on the object-side surface or image-side surface of other lenses is denoted in the same manner

The lens parameter related to an aberration:

Optical distortion for image formation in the optical image capturing system is denoted by ODT. TV distortion for image formation in the optical image capturing system is denoted by TDT. Further, the range of the aberration offset for the view of image formation may be limited to 50%-100% field. An offset of the spherical aberration is denoted by DFS. An offset of the coma aberration is denoted by DFC.

Transverse aberration on an edge of an aperture is denoted by STA, which stands for STOP transverse aberration, and is used to evaluate the performance of one specific optical image capturing system. The transverse aberration of light in any field of view can be calculated with a tangential fan or a sagittal fan. More specifically, the transverse aberration caused when the longest operation wavelength (e.g., 940 nm or 960 nm) and the shortest operation wavelength (e.g., 840 nm or 850 nm) pass through the edge of the aperture can be used as the reference for evaluating performance. The coordinate directions of the aforementioned tangential fan can be further divided into a positive direction (upper light) and a negative direction (lower light). The longest operation wavelength which passes through the edge of the aperture has an imaging position on the image plane specifically for the infrared light in a particular field of view, and the reference wavelength of the mail light (e.g., 940 nm) has another imaging position on the image plane specifically for the infrared light in the same field of view. The transverse aberration caused when the longest operation wavelength passes through the edge of the aperture is defined as a distance between these two imaging positions. Similarly, the shortest operation wavelength which passes through the edge of the aperture has an imaging position on the image plane specifically for the infrared light in a particular field of view, and the transverse aberration caused when the shortest operation wavelength passes through the edge of the aperture is defined as a distance between the imaging position of the shortest operation wavelength and the imaging position of the reference wavelength. The performance of the optical image capturing system can be considered excellent if the transverse aberrations of the shortest and the longest operation wavelength which pass through the edge of the aperture and image on the image plane specifically for the infrared light in 0.7 field of view (i.e., 0.7 times the height for image formation HOI) are both less than 100 μm. Furthermore, for a stricter evaluation, the performance cannot be considered excellent unless the transverse aberrations of the shortest and the longest operation wavelength which pass through the edge of the aperture and image on the image plane specifically for the infrared light in 0.7 field of view are both less than 80 μm.

The optical image capturing system has a maximum image height HOI on the image plane specifically for the infrared light which is vertical to the optical axis. A transverse aberration at 0.7 HOI in the positive direction of the tangential fan after the longest operation wavelength of infrared light passing through the edge of the aperture is denoted by PLTA; a transverse aberration at 0.7 HOI in the positive direction of the tangential fan after the shortest operation wavelength of infrared light passing through the edge of the aperture is denoted by PSTA; a transverse aberration at 0.7 HOI in the negative direction of the tangential fan after the longest operation wavelength of infrared light passing through the edge of the aperture is denoted by NLTA; a transverse aberration at 0.7 HOI in the negative direction of the tangential fan after the shortest operation wavelength of infrared light passing through the edge of the aperture is denoted by NSTA; a transverse aberration at 0.7 HOI of the sagittal fan after the longest operation wavelength of infrared light passing through the edge of the aperture is denoted by SLTA; a transverse aberration at 0.7 HOI of the sagittal fan after the shortest operation wavelength of infrared light passing through the edge of the aperture is denoted by SSTA.

The present invention provides an optical image capturing system, in which the seventh lens is provided with an inflection point at the object-side surface or at the image-side surface to adjust the incident angle of each view field and modify the ODT and the TDT. In addition, the surfaces of the seventh lens are capable of modifying the optical path to improve the imagining quality.

The optical image capturing system of the present invention includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane specifically for the infrared light in order along an optical axis from an object side to an image side. All of the first lens to the seventh lens have refractive power. The optical image capturing system satisfies:

0.5≤f/HEP≤1.8; 0 deg<HAF≤50 deg; and 0.9≤2(ARE/HEP)≤2.0;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengths of the first lens to the seventh lens; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HXP is an exit pupil diameter of the image-side surface of the seventh lens; HOS is a distance between an object-side surface, which face the object side, of the first lens and the image plane specifically for the infrared light on the optical axis; HAF is a half of the maximum field angle; HOI is a maximum height for image formation of the optical image capturing system; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the exit pupil diameter away from the optical axis.

The present invention further provides an optical image capturing system, including a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane specifically for the infrared light in order along an optical axis from an object side to an image side. At least one surface of at least one lens among the first lens to the seventh lens has at least an inflection point thereon. The optical image capturing system satisfies:

0.5≤f/HEP≤1.5; 0 deg<HAF≤50 deg; and 0.9≤2(ARE/HEP)≤2.0;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengths of the first lens to the seventh lens; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HXP is an exit pupil diameter of the image-side surface of the seventh lens; HOS is a distance between an object-side surface, which face the object side, of the first lens and the image plane specifically for the infrared light on the optical axis; InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens on the optical axis; HAF is a half of the maximum field angle; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the exit pupil diameter away from the optical axis.

The present invention further provides an optical image capturing system, including a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane specifically for the infrared light, in order along an optical axis from an object side to an image side. The number of the lenses having refractive power in the optical image capturing system is seven. At least one surface of at least two lenses among the first lens to the seventh lens has at least an inflection point thereon. The optical image capturing system satisfies:

0.5≤f/HEP≤1.3; 10 deg<HAF≤50 deg; and 0.9≤2(ARE/HEP)≤2.0;

wherein f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis between an object-side surface, which face the object side, of the first lens and the image plane specifically for the infrared light; HOI is a maximum height for image formation of the optical image capturing system; HAF is a half of the maximum field angle; HXP is an exit pupil diameter of the image-side surface of the seventh lens; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the exit pupil diameter away from the optical axis.

For any surface of any lens, the profile curve length within the effective half diameter affects the ability of the surface to correct aberration and differences between optical paths of light in different fields of view. With longer profile curve length, the ability to correct aberration is better. However, the difficulty of manufacturing increases as well. Therefore, the profile curve length within the effective half diameter of any surface of any lens has to be controlled. The ratio between the profile curve length (ARS) within the effective half diameter of one surface and the thickness (TP) of the lens, which the surface belonged to, on the optical axis (i.e., ARS/TP) has to be particularly controlled. For example, the profile curve length of the maximum effective half diameter of the object-side surface of the first lens is denoted by ARS11, the thickness of the first lens on the optical axis is TP1, and the ratio between these two parameters is ARS11/TP1; the profile curve length of the maximum effective half diameter of the image-side surface of the first lens is denoted by ARS12, and the ratio between ARS12 and TP1 is ARS12/TP1. The profile curve length of the maximum effective half diameter of the object-side surface of the second lens is denoted by ARS21, the thickness of the second lens on the optical axis is TP2, and the ratio between these two parameters is ARS21/TP2; the profile curve length of the maximum effective half diameter of the image-side surface of the second lens is denoted by ARS22, and the ratio between ARS22 and TP2 is ARS22/TP2. For any surface of other lenses in the optical image capturing system, the ratio between the profile curve length of the maximum effective half diameter thereof and the thickness of the lens which the surface belonged to is denoted in the same manner.

For any surface of any lens, the profile curve length within a half of the entrance pupil diameter (HEP) affects the ability of the surface to correct aberration and differences between optical paths of light in different fields of view. With longer profile curve length, the ability to correct aberration is better. However, the difficulty of manufacturing increases as well. Therefore, the profile curve length within a half of the entrance pupil diameter (HEP) of any surface of any lens has to be controlled. The ratio between the profile curve length (ARE) within a half of the entrance pupil diameter (HEP) of one surface and the thickness (TP) of the lens, which the surface belonged to, on the optical axis (i.e., ARE/TP) has to be particularly controlled. For example, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the first lens is denoted by ARE11, the thickness of the first lens on the optical axis is TP1, and the ratio between these two parameters is ARE11/TP1; the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens is denoted by ARE12, and the ratio between ARE12 and TP1 is ARE12/TP1. The profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the second lens is denoted by ARE21, the thickness of the second lens on the optical axis is TP2, and the ratio between these two parameters is ARE21/TP2; the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens is denoted by ARE22, and the ratio between ARE22 and TP2 is ARE22/TP2. For any surface of other lenses in the optical image capturing system, the ratio between the profile curve length of a half of the entrance pupil diameter (HEP) thereof and the thickness of the lens which the surface belonged to is denoted in the same manner.

In an embodiment, a height of the optical image capturing system (HOS) can be reduced if |f1|>|f7|.

In an embodiment, when |f2|+|f3|+|f4|+|f5|+|f6| and |f1|+|f7| of the lenses satisfy the aforementioned conditions, at least one lens among the second to the sixth lenses could have weak positive refractive power or weak negative refractive power. Herein the weak refractive power means the absolute value of the focal length of one specific lens is greater than 10. When at least one lens among the second to the sixth lenses has weak positive refractive power, it may share the positive refractive power of the first lens, and on the contrary, when at least one lens among the second to the sixth lenses has weak negative refractive power, it may fine turn and correct the aberration of the system.

In an embodiment, the seventh lens could have negative refractive power, and an image-side surface thereof is concave, it may reduce back focal length and size. Besides, the seventh lens can have at least an inflection point on at least a surface thereof, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The present invention will be best understood by referring to the following detailed description of some illustrative embodiments in conjunction with the accompanying drawings, in which

FIG. 1A is a schematic diagram of a first embodiment of the present invention;

FIG. 1B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the first embodiment of the present application;

FIG. 1C shows a tangential fan and a sagittal fan of the optical image capturing system of the first embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 2A is a schematic diagram of a second embodiment of the present invention;

FIG. 2B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the second embodiment of the present application;

FIG. 2C shows a tangential fan and a sagittal fan of the optical image capturing system of the second embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 3A is a schematic diagram of a third embodiment of the present invention;

FIG. 3B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the third embodiment of the present application;

FIG. 3C shows a tangential fan and a sagittal fan of the optical image capturing system of the third embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 4A is a schematic diagram of a fourth embodiment of the present invention;

FIG. 4B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the fourth embodiment of the present application;

FIG. 4C shows a tangential fan and a sagittal fan of the optical image capturing system of the fourth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 5A is a schematic diagram of a fifth embodiment of the present invention;

FIG. 5B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the fifth embodiment of the present application;

FIG. 5C shows a tangential fan and a sagittal fan of the optical image capturing system of the fifth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 6A is a schematic diagram of a sixth embodiment of the present invention;

FIG. 6B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the sixth embodiment of the present application; and

FIG. 6C shows a tangential fan and a sagittal fan of the optical image capturing system of the sixth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture.

DETAILED DESCRIPTION OF THE INVENTION

An optical image capturing system of the present invention includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane specifically for the infrared light from an object side to an image side. The optical image capturing system further includes an image sensor disposed at the image plane specifically for the infrared light, wherein the image heights of the following embodiments are all around 3.91 mm.

The optical image capturing system could work in three infrared light wavelengths, including 850 nm, 940 nm, and 960 nm, wherein 960 nm is the main reference wavelength and is the reference wavelength for obtaining the technical characters.

The optical image capturing system could work in three visible light wavelengths, including 486.1 nm, 587.5 nm, and 656.2 nm, wherein 587.5 nm is the main reference wavelength and is the reference wavelength for obtaining the technical characters. The optical image capturing system could also work in five wavelengths, including 470 nm, 510 nm, 555 nm, 610 nm, and 650 nm wherein 555 nm is the main reference wavelength, and is the reference wavelength for obtaining the visible light technical characters.

The optical image capturing system of the present invention satisfies 0.5≤ΣPPR/|ΣNPR|≤15, and a preferable range is 1≤ΣPPR/|ΣNPR|≤3.0, where PPR is a ratio of the focal length f of the optical image capturing system to a focal length fp of each of lenses with positive refractive power; NPR is a ratio of the focal length f of the optical image capturing system to a focal length fn of each of lenses with negative refractive power; ΣPPR is a sum of the PPRs of each positive lens; and ΣNPR is a sum of the NPRs of each negative lens. It is helpful for control of an entire refractive power and an entire length of the optical image capturing system.

The image sensor is provided on the image plane, and is provided with at least one hundred thousand pixels. The optical image capturing system of the present invention satisfies HOS/HOI≤10; and 0.5≤HOS/f≤10, and a preferable range is 1≤HOS/HOI≤5; and 1≤HOS/f≤7, where HOI is a half of a diagonal of an effective sensing area of the image sensor, i.e., the maximum image height, and HOS is a height of the optical image capturing system, i.e. a distance on the optical axis between the object-side surface of the first lens and the image plane specifically for the infrared light. It is helpful for reduction of the size of the system for used in compact cameras.

The optical image capturing system of the present invention further is provided with an aperture to increase image quality.

In the optical image capturing system of the present invention, the aperture could be a front aperture or a middle aperture, wherein the front aperture is provided between the object and the first lens, and the middle is provided between the first lens and the image plane specifically for the infrared light. The front aperture provides a long distance between an exit pupil of the system and the image plane specifically for the infrared light, which allows more elements to be installed. The middle could enlarge a view angle of view of the system and increase the efficiency of the image sensor. The optical image capturing system satisfies 0.2≤InS/HOS≤1.1, where InS is a distance between the aperture and the image-side surface of the sixth lens. It is helpful for size reduction and wide angle.

The optical image capturing system of the present invention satisfies 0.1≤ΣTP/InTL≤0.9, where InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens, and ΣTP is a sum of central thicknesses of the lenses on the optical axis. It is helpful for the contrast of image and yield rate of manufacture and provides a suitable back focal length for installation of other elements.

The optical image capturing system of the present invention satisfies 0.001≤|R1/R2|≤20, and a preferable range is 0.01≤|R1/R2|<10, where R1 is a radius of curvature of the object-side surface of the first lens, and R2 is a radius of curvature of the image-side surface of the first lens. It provides the first lens with a suitable positive refractive power to reduce the increase rate of the spherical aberration.

The optical image capturing system of the present invention satisfies −7<(R13−R14)/(R13+R14)<50, where R13 is a radius of curvature of the object-side surface of the seventh lens, and R14 is a radius of curvature of the image-side surface of the seventh lens. It may modify the astigmatic field curvature.

The optical image capturing system of the present invention satisfies IN12/f≤3.0, where IN12 is a distance on the optical axis between the first lens and the second lens. It may correct chromatic aberration and improve the performance.

The optical image capturing system of the present invention satisfies IN67/f≤0.8, where IN67 is a distance on the optical axis between the sixth lens and the seventh lens. It may correct chromatic aberration and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≤(TP1+IN12)/TP2≤10, where TP1 is a central thickness of the first lens on the optical axis, and TP2 is a central thickness of the second lens on the optical axis. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≤(TP7+IN67)/TP6≤10, where TP6 is a central thickness of the sixth lens on the optical axis, TP7 is a central thickness of the seventh lens on the optical axis, and IN67 is a distance between the sixth lens and the seventh lens. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≤TP4/(IN34+TP4+IN45)<1, where TP3 is a central thickness of the third lens on the optical axis, TP4 is a central thickness of the fourth lens on the optical axis, TP5 is a central thickness of the fifth lens on the optical axis, IN34 is a distance on the optical axis between the third lens and the fourth lens, IN45 is a distance on the optical axis between the fourth lens and the fifth lens, and InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens. It may fine tune and correct the aberration of the incident rays layer by layer, and reduce the height of the system.

The optical image capturing system satisfies 0 mm≤HVT71≤3 mm; 0 mm<HVT72≤6 mm; 0≤HVT71/HVT72; 0 mm≤|SGC71|≤0.5 mm; 0 mm<|SGC72|≤2 mm; and 0<|SGC72|/(|SGC72|+TP7)≤0.9, where HVT71 a distance perpendicular to the optical axis between the critical point C71 on the object-side surface of the seventh lens and the optical axis; HVT72 a distance perpendicular to the optical axis between the critical point C72 on the image-side surface of the seventh lens and the optical axis; SGC71 is a distance on the optical axis between a point on the object-side surface of the seventh lens where the optical axis passes through and a point where the critical point C71 projects on the optical axis; SGC72 is a distance on the optical axis between a point on the image-side surface of the seventh lens where the optical axis passes through and a point where the critical point C72 projects on the optical axis. It is helpful to correct the off-axis view field aberration.

The optical image capturing system satisfies 0.2≤HVT72/HOI≤0.9, and preferably satisfies 0.3≤HVT72/HOI≤0.8. It may help to correct the peripheral aberration.

The optical image capturing system satisfies 0≤HVT72/HOS≤0.5, and preferably satisfies 0.2≤HVT72/HOS≤0.45. It may help to correct the peripheral aberration.

The optical image capturing system of the present invention satisfies 0<SGI711/(SGI711+TP7)≤0.9; 0<SGI721/(SGI721+TP7)≤0.9, and it is preferable to satisfy 0.1≤SGI711/(SGI711+TP7)≤0.6; 0.1≤SGI721/(SGI721+TP7)≤0.6, where SGI711 is a displacement on the optical axis from a point on the object-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI721 is a displacement on the optical axis from a point on the image-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

The optical image capturing system of the present invention satisfies 0<SGI712/(SGI712+TP7)≤0.9; 0<SGI722/(SGI722+TP7)≤0.9, and it is preferable to satisfy 0.1≤SGI712/(SGI712+TP7)≤0.6; 0.1<SGI722/(SGI722+TP7)≤0.6, where SGI712 is a displacement on the optical axis from a point on the object-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI722 is a displacement on the optical axis from a point on the image-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF711|≤5 mm; 0.001 mm≤|HIF721|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF711|≤3.5 mm; 1.5 mm≤|HIF721|≤3.5 mm, where HIF711 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis; HIF721 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF712|≤5 mm; 0.001 mm≤|HIF722|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF722|≤3.5 mm; 0.1 mm≤|HIF712|≤3.5 mm, where HIF712 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the second closest to the optical axis, and the optical axis; HlF722 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the second closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF713|≤5 mm; 0.001 mm≤|HIF723|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF723|≤3.5 mm; 0.1 mm≤|HIF713|≤3.5 mm, where HIF713 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the third closest to the optical axis, and the optical axis; HIF723 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the third closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF714|≤5 mm; 0.001 mm≤|HIF724|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF724|≤3.5 mm; 0.1 mm≤|HIF714|≤3.5 mm, where HIF714 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the fourth closest to the optical axis, and the optical axis; HIF724 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the fourth closest to the optical axis, and the optical axis.

In an embodiment, the lenses of high Abbe number and the lenses of low Abbe number are arranged in an interlaced arrangement that could be helpful for correction of aberration of the system.

An equation of aspheric surface is

z=ch ²/[1+[1−(k+1)c ² h ²]^(0.5)]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹² +A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+ . . .   (1)

where z is a depression of the aspheric surface; k is conic constant; c is reciprocal of the radius of curvature; and A4, A6, A8, A10, A12, A14, A16, A18, and A20 are high-order aspheric coefficients.

In the optical image capturing system, the lenses could be made of plastic or glass. The plastic lenses may reduce the weight and lower the cost of the system, and the glass lenses may control the thermal effect and enlarge the space for arrangement of the refractive power of the system. In addition, the opposite surfaces (object-side surface and image-side surface) of the first to the seventh lenses could be aspheric that can obtain more control parameters to reduce aberration. The number of aspheric glass lenses could be less than the conventional spherical glass lenses, which is helpful for reduction of the height of the system.

When the lens has a convex surface, which means that the surface is convex around a position, through which the optical axis passes, and when the lens has a concave surface, which means that the surface is concave around a position, through which the optical axis passes.

The optical image capturing system of the present invention could be applied in a dynamic focusing optical system. It is superior in the correction of aberration and high imaging quality so that it could be allied in lots of fields.

The optical image capturing system of the present invention could further include a driving module to meet different demands, wherein the driving module can be coupled with the lenses to move the lenses. The driving module can be a voice coil motor (VCM), which is used to move the lens for focusing, or can be an optical image stabilization (OIS) component, which is used to lower the possibility of having the problem of image blurring which is caused by subtle movements of the lens while shooting.

To meet different requirements, at least one lens among the first lens to the seventh lens of the optical image capturing system of the present invention can be a light filter, which filters out light of wavelength shorter than 500 nm. Such effect can be achieved by coating on at least one surface of the lens, or by using materials capable of filtering out short waves to make the lens.

To meet different requirements, the image plane specifically for the infrared light of the optical image capturing system in the present invention can be either flat or curved. If the image plane specifically for the infrared light is curved (e.g., a sphere with a radius of curvature), the incidence angle required for focusing light on the image plane specifically for the infrared light can be decreased, which is not only helpful to shorten the length of the system (TTL), but also helpful to increase the relative illuminance.

The optical image capturing system of the present invention could be applied to three-dimensional image capture. A light with specific characteristics is projected onto an object, and is reflected by a surface of the object, and is then received and calculated and analyzed by the lens to obtain the distance between each position of the object and the lens, thereby to determine the information of the three-dimensional image. The light projection usually uses infrared rays in a specific wavelength to reduce interference, thereby to achieving more accurate measurement. The detecting way for capturing the three-dimensional image could be, but not limited to, technologies such as time-of-flight (TOF) or structured light.

We provide several embodiments in conjunction with the accompanying drawings for the best understanding, which are:

First Embodiment

As shown in FIG. 1A and FIG. 1B, an optical image capturing system 10 of the first embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 110, a second lens 120, a third lens 130, an aperture 100, a fourth lens 140, a fifth lens 150, a sixth lens 160, a seventh lens 170, an infrared rays filter 180, an image plane specifically for the infrared light 190, and an image sensor 192. FIG. 1C shows a tangential fan and a sagittal fan of the optical image capturing system 10 of the first embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of the aperture 100.

The first lens 110 has negative refractive power and is made of plastic. An object-side surface 112 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 114 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 112 has an inflection point, and the image-side surface 114 has two inflection points. A profile curve length of the maximum effective half diameter of an object-side surface of the first lens 110 is denoted by ARS11, and a profile curve length of the maximum effective half diameter of the image-side surface of the first lens 110 is denoted by ARS12. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the first lens 110 is denoted by ARE11, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens 110 is denoted by ARE12. A thickness of the first lens 110 on the optical axis is TP1.

The first lens 110 satisfies SGI111=−0.1110 mm; SGI121=2.7120 mm; TP1=2.2761 mm; |SGI111|/(|SGI111|+TP1)=0.0465; |SGI121|/(|SGI121|+TP1)=0.5437, where a displacement on the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis, is denoted by SGI111, and a displacement on the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis is denoted by SGI121.

The first lens 110 satisfies SGI112=0 mm; SGI122=4.2315 mm; |SGI112|/(|SGI112|+TP1)=0; |SGI122|/(|SGI122|+TP1)=0.6502, where a displacement on the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the second closest to the optical axis, projects on the optical axis, is denoted by SGI112, and a displacement on the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the second closest to the optical axis, projects on the optical axis is denoted by SGI122.

The first lens 110 satisfies HIF111=12.8432 mm; HIF111/ HOI=1.7127; HIF121=7.1744 mm; HIF121/HOI=0.9567, where a displacement perpendicular to the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF111, and a displacement perpendicular to the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF121.

The first lens 110 satisfies HIF112=0 mm; HIF112/HOI=0; HIF122=9.8592 mm; HIF122/HOI=1.3147, where a displacement perpendicular to the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the second closest to the optical axis is denoted by HIF112, and a displacement perpendicular to the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the second closest to the optical axis is denoted by HIF122.

The second lens 120 has positive refractive power and is made of plastic. An object-side surface 122 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 124 thereof, which faces the image side, is a concave aspheric surface. A profile curve length of the maximum effective half diameter of an object-side surface of the second lens 120 is denoted by ARS21, and a profile curve length of the maximum effective half diameter of the image-side surface of the second lens 120 is denoted by ARS22. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the second lens 120 is denoted by ARE21, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens 120 is denoted by ARE22. A thickness of the second lens 120 on the optical axis is TP2.

For the second lens 120, a displacement on the optical axis from a point on the object-side surface of the second lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis, is denoted by SGI211, and a displacement on the optical axis from a point on the image-side surface of the second lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis is denoted by SGI221.

For the second lens, a displacement perpendicular to the optical axis from a point on the object-side surface of the second lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF211, and a displacement perpendicular to the optical axis from a point on the image-side surface of the second lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF221.

The third lens 130 has negative refractive power and is made of plastic. An object-side surface 132, which faces the object side, is a convex aspheric surface, and an image-side surface 134, which faces the image side, is a concave aspheric surface. A profile curve length of the maximum effective half diameter of an object-side surface of the third lens 130 is denoted by ARS31, and a profile curve length of the maximum effective half diameter of the image-side surface of the third lens 130 is denoted by ARS32. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the third lens 130 is denoted by ARE31, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the third lens 130 is denoted by ARE32. A thickness of the third lens 130 on the optical axis is TP3.

For the third lens 130, SGI311 is a displacement on the optical axis from a point on the object-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI321 is a displacement on the optical axis from a point on the image-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

For the third lens 130, SGI312 is a displacement on the optical axis from a point on the object-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI322 is a displacement on the optical axis from a point on the image-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

For the third lens 130, HIF311 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens, which is the closest to the optical axis, and the optical axis; HIF321 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the third lens, which is the closest to the optical axis, and the optical axis.

For the third lens 130, HIF312 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens, which is the second closest to the optical axis, and the optical axis; HIF322 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the third lens, which is the second closest to the optical axis, and the optical axis.

The fourth lens 140 has positive refractive power and is made of plastic. An object-side surface 142, which faces the object side, is a convex aspheric surface, and an image-side surface 144, which faces the image side, is a convex aspheric surface. The object-side surface 142 has an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the fourth lens 140 is denoted by ARS41, and a profile curve length of the maximum effective half diameter of the image-side surface of the fourth lens 140 is denoted by ARS42. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the fourth lens 140 is denoted by ARE41, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the fourth lens 140 is denoted by ARE42. A thickness of the fourth lens 140 on the optical axis is TP4.

The fourth lens 140 satisfies SGI411=0.0018 mm; |SGI411|/(|SGI411|+TP4)=0.0009, where SGI411 is a displacement on the optical axis from a point on the object-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI421 is a displacement on the optical axis from a point on the image-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

For the fourth lens 140, SGI412 is a displacement on the optical axis from a point on the object-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI422 is a displacement on the optical axis from a point on the image-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

The fourth lens 140 further satisfies HIF411=0.7191 mm; HIF411/HOI=0.0959, where HIF411 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens, which is the closest to the optical axis, and the optical axis; HIF421 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens, which is the closest to the optical axis, and the optical axis.

For the fourth lens 140, HIF412 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens, which is the second closest to the optical axis, and the optical axis; HIF422 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens, which is the second closest to the optical axis, and the optical axis.

The fifth lens 150 has positive refractive power and is made of plastic. An object-side surface 152, which faces the object side, is a concave aspheric surface, and an image-side surface 154, which faces the image side, is a convex aspheric surface. The object-side surface 152 and the image-side surface 154 both have an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the fifth lens 150 is denoted by ARS51, and a profile curve length of the maximum effective half diameter of the image-side surface of the fifth lens 150 is denoted by ARS52. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the fifth lens 150 is denoted by ARE51, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the fifth lens 150 is denoted by ARE52. A thickness of the fifth lens 150 on the optical axis is TPS.

The fifth lens 150 satisfies SGI511=−0.1246 mm; SGI521=−2.1477 mm; |SGI511|/(|SGI511|+TP5)=0.0284; |SGI521|/(|SGI521|+TP5)=0.3346, where SGI511 is a displacement on the optical axis from a point on the object-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI521 is a displacement on the optical axis from a point on the image-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

For the fifth lens 150, SGI512 is a displacement on the optical axis from a point on the object-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI522 is a displacement on the optical axis from a point on the image-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

The fifth lens 150 further satisfies HIF511=3.8179 mm; HIF521=4.5480 mm; HIF511/HOI=0.5091; HIF521/HOI=0.6065, where HIF511 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fifth lens, which is the closest to the optical axis, and the optical axis; HIF521 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fifth lens, which is the closest to the optical axis, and the optical axis.

For the fifth lens 150, HIF512 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fifth lens, which is the second closest to the optical axis, and the optical axis; HIF522 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fifth lens, which is the second closest to the optical axis, and the optical axis.

The sixth lens 160 has negative refractive power and is made of plastic. An object-side surface 162, which faces the object side, is a convex surface, and an image-side surface 164, which faces the image side, is a concave surface. The object-side surface 162 and the image-side surface 164 both have an inflection point. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration. A profile curve length of the maximum effective half diameter of an object-side surface of the sixth lens 160 is denoted by ARS61, and a profile curve length of the maximum effective half diameter of the image-side surface of the sixth lens 160 is denoted by ARS62. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the sixth lens 160 is denoted by ARE61, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the sixth lens 160 is denoted by ARE62. A thickness of the sixth lens 160 on the optical axis is TP6.

The sixth lens 160 satisfies SGI611=0.3208 mm; SGI621=0.5937 mm; |SGI611|/(|SGI611|+TP6)=0.5167; |SGI621|/(|SGI621|+TP6)=0.6643, where SGI611 is a displacement on the optical axis from a point on the object-side surface of the sixth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI621 is a displacement on the optical axis from a point on the image-side surface of the sixth lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

The sixth lens 160 further satisfies HIF611=1.9655 mm; HIF621=2.0041 mm; HIF611/HOI=0.2621; HIF621/HOI=0.2672, where HIF611 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the sixth lens, which is the closest to the optical axis, and the optical axis; HIF621 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the sixth lens, which is the closest to the optical axis, and the optical axis.

The seventh lens 170 has positive refractive power and is made of plastic. An object-side surface 172, which faces the object side, is a convex surface, and an image-side surface 174, which faces the image side, is a concave surface. Whereby, it is helpful to shorten the focal length behind the seventh lens for miniaturization. The object-side surface 172 and the image-side surface 174 both have an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the seventh lens 170 is denoted by ARS71, and a profile curve length of the maximum effective half diameter of the image-side surface of the seventh lens 170 is denoted by ARS72. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the seventh lens 170 is denoted by ARE71, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the seventh lens 170 is denoted by ARE72. A thickness of the seventh lens 170 on the optical axis is TP7.

The seventh lens 170 satisfies SGI711=0.5212 mm; SGI721=0.5668 mm; |SGI711|/(|SGI711|+TP7)=0.3179; |SGI721|/(|SGI721|+TP7)=0.3364, where SGI711 is a displacement on the optical axis from a point on the object-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI721 is a displacement on the optical axis from a point on the image-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

The seventh lens 170 further satisfies HIF711=1.6707 mm; HIF721=1.8616 mm; HIF711/HOI=0.2228; HIF721/HOI=0.2482, where HIF711 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis; HIF721 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis.

The features related to the inflection points in the present embodiment described below are obtained with the main reference wavelength 555 nm.

The infrared rays filter 180 is made of glass and between the seventh lens 170 and the image plane specifically for the infrared light 190. The infrared rays filter 180 gives no contribution to the focal length of the system.

The optical image capturing system 10 of the first embodiment has the following parameters, which are f=4.3019 mm; f/HEP=1.2; HAF=59.9968; and tan(HAF)=1.7318, where f is a focal length of the system; HAF is a half of the maximum field angle; and HEP is an entrance pupil diameter.

The parameters of the lenses of the first embodiment are f1=−14.5286 mm; |f/f1|=0.2961; f7=8.2933; |f1|>f7; and |f1/f7|=1.7519, where f1 is a focal length of the first lens 110; and f7 is a focal length of the seventh lens 170.

The first embodiment further satisfies |f2|+|f3|+|f4|+|f5|+|f6|=144.7494; |f1|+|f7|=22.8219 and |f2|+|f3|+|f4|+|f5|+|f6|>|f1|+|f7|, where f2 is a focal length of the second lens 120, f3 is a focal length of the third lens 130, f4 is a focal length of the fourth lens 140, f5 is a focal length of the fifth lens 150, f6 is a focal length of the sixth lens 160, and f7 is a focal length of the seventh lens 170.

The optical image capturing system 10 of the first embodiment further satisfies ΣPPR=f/f2+f/f4+f/f5+f/f7=1.7384; ΣNPR=f/f1+f/f3+f/f6=−0.9999; ΣPPR/|ΣNPR|=1.7386; |f/f2|=0.1774; |f/f3|=0.0443; |f/f4|=0.4411; |f/f5|=0.6012; |f/f6|=0.6595; |f/f7|=0.5187, where PPR is a ratio of a focal length f of the optical image capturing system to a focal length fp of each of the lenses with positive refractive power; and NPR is a ratio of a focal length f of the optical image capturing system to a focal length fn of each of lenses with negative refractive power.

The optical image capturing system 10 of the first embodiment further satisfies InTL+BFL=HOS; HOS=26.9789 mm; HOI=7.5 mm; HOS/HOI=3.5977; HOS/f=6.2715; InS=12.4615 mm; and InS/HOS=0.4619, where InTL is a distance between the object-side surface 112 of the first lens 110 and the image-side surface 174 of the seventh lens 170; HOS is a height of the image capturing system, i.e. a distance between the object-side surface 112 of the first lens 110 and the image plane specifically for the infrared light 190; InS is a distance between the aperture 100 and the image plane specifically for the infrared light 190; HOI is a half of a diagonal of an effective sensing area of the image sensor 192, i.e., the maximum image height; and BFL is a distance between the image-side surface 174 of the seventh lens 170 and the image plane specifically for the infrared light 190.

The optical image capturing system 10 of the first embodiment further satisfies ΣTP=16.0446 mm; and ΣTP/InTL=0.6559, where ΣTP is a sum of the thicknesses of the lenses 110-170 with refractive power. It is helpful for the contrast of image and yield rate of manufacture and provides a suitable back focal length for installation of other elements.

The optical image capturing system 10 of the first embodiment further satisfies |R1/R2|=129.9952, where R1 is a radius of curvature of the object-side surface 112 of the first lens 110, and R2 is a radius of curvature of the image-side surface 114 of the first lens 110. It provides the first lens with a suitable positive refractive power to reduce the increase rate of the spherical aberration.

The optical image capturing system 10 of the first embodiment further satisfies (R13−R14)/(R13+R14)=−0.0806, where R13 is a radius of curvature of the object-side surface 172 of the seventh lens 170, and R14 is a radius of curvature of the image-side surface 174 of the seventh lens 170. It may modify the astigmatic field curvature.

The optical image capturing system 10 of the first embodiment further satisfies ΣPP=f2+f4+f5+f7=49.4535 mm; and f4/(f2+f4+f5+f7)=0.1972, where ΣPP is a sum of the focal lengths fp of each lens with positive refractive power. It is helpful to share the positive refractive power of the fourth lens 140 to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment further satisfies ΣNP=f1+f3+f6=−118.1178 mm; and f1/(f1+f3+f6)=0.1677, where ΣNP is a sum of the focal lengths fn of each lens with negative refractive power. It is helpful to share the negative refractive power of the first lens 110 to other negative lenses, which avoids the significant aberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment further satisfies IN12=4.5524 mm; IN12/f=1.0582, where IN12 is a distance on the optical axis between the first lens 110 and the second lens 120. It may correct chromatic aberration and improve the performance.

The optical image capturing system 10 of the first embodiment further satisfies TP1=2.2761 mm; TP2=0.2398 mm; and (TP1+IN12)/TP2=1.3032, where TP1 is a central thickness of the first lens 110 on the optical axis, and TP2 is a central thickness of the second lens 120 on the optical axis. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system 10 of the first embodiment further satisfies TP6=0.3000 mm; TP7=1.1182 mm; and (TP7+IN67)/TP6=4.4322, where TP6 is a central thickness of the sixth lens 160 on the optical axis, TP7 is a central thickness of the seventh lens 170 on the optical axis, and IN67 is a distance on the optical axis between the sixth lens 160 and the seventh lens 170. It may control the sensitivity of manufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment further satisfies TP3=0.8369 mm; TP4=2.0022 mm; TP5=4.2706 mm; IN34=1.9268 mm; IN45=1.5153 mm; and TP4/(IN34+TP4+IN45)=0.3678, where TP3 is a central thickness of the third lens 130 on the optical axis, TP4 is a central thickness of the fourth lens 140 on the optical axis, TP5 is a central thickness of the fifth lens 150 on the optical axis, IN34 is a distance on the optical axis between the third lens 130 and the fourth lens 140, and IN45 is a distance on the optical axis between the fourth lens 140 and the fifth lens 150. It may control the sensitivity of manufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment further satisfies InRS61=−0.7823 mm; InRS62=−0.2166 mm; and |InRS62|/TP6=0.722, where InRS61 is a displacement from a point on the object-side surface 162 of the sixth lens 160 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the object-side surface 162 of the sixth lens 160 ends; InRS62 is a displacement from a point on the image-side surface 164 of the sixth lens 160 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the image-side surface 164 of the sixth lens 160 ends; and TP6 is a central thickness of the sixth lens 160 on the optical axis. It is helpful for manufacturing and shaping of the lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment further satisfies HVT61=3.3498 mm; HVT62=3.9860 mm; and HVT61/HVT62=0.8404, where HVT61 a distance perpendicular to the optical axis between the critical point on the object-side surface 162 of the sixth lens 160 and the optical axis; and HVT62 a distance perpendicular to the optical axis between the critical point on the image-side surface 164 of the sixth lens 160 and the optical axis.

The optical image capturing system 10 of the first embodiment further satisfies InRS71=−0.2756 mm; InRS72=−0.0938 mm; and |InRS72|/TP7=0.0839, where InRS71 is a displacement from a point on the object-side surface 172 of the seventh lens 170 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the object-side surface 172 of the seventh lens 170 ends; InRS72 is a displacement from a point on the image-side surface 174 of the seventh lens 170 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the image-side surface 174 of the seventh lens 170 ends; and TP7 is a central thickness of the seventh lens 170 on the optical axis. It is helpful for manufacturing and shaping of the lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment satisfies HVT71=3.6822 mm; HVT72=4.0606 mm; and HVT71/HVT72=0.9068, where HVT71 a distance perpendicular to the optical axis between the critical point on the object-side surface 172 of the seventh lens 170 and the optical axis; and HVT72 a distance perpendicular to the optical axis between the critical point on the image-side surface 174 of the seventh lens 170 and the optical axis.

The optical image capturing system 10 of the first embodiment satisfies HVT72/HOI=0.5414. It is helpful for correction of the aberration of the peripheral view field of the optical image capturing system.

The optical image capturing system 10 of the first embodiment satisfies HVT72/HOS=0.1505. It is helpful for correction of the aberration of the peripheral view field of the optical image capturing system.

The second lens 120, the third lens 130, and the seventh lens 170 have negative refractive power. The optical image capturing system 10 of the first embodiment further satisfies 1≤NA7/NA2, where NA2 is an Abbe number of the second lens 120; and NA7 is an Abbe number of the seventh lens 170. It may correct the aberration of the optical image capturing system.

The optical image capturing system 10 of the first embodiment further satisfies |TDT|=2.5678%; |ODT|=2.1302%, where TDT is TV distortion; and ODT is optical distortion.

For the fifth lens 150 of the optical image capturing system 10 in the first embodiment, a transverse aberration at 0.7 field of view in the positive direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by PSTA, and is 0.00040 mm; a transverse aberration at 0.7 field of view in the positive direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by PLTA, and is −0.009 mm; a transverse aberration at 0.7 field of view in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by NSTA, and is −0.002 mm; a transverse aberration at 0.7 field of view in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by NLTA, and is −0.016 mm; a transverse aberration at 0.7 field of view of the sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by SSTA, and is 0.018 mm; a transverse aberration at 0.7 field of view of the sagittal fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by SLTA, and is 0.016 mm.

The parameters of the lenses of the first embodiment are listed in Table 1 and Table 2.

TABLE 1 f = 4.3019 mm; f/HEP = 1.2; HAF = 59.9968 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens −1079.499964 2.276 plastic 1.565 58.00 −14.53 2 8.304149657 4.552 3 2^(nd) lens 14.39130913 5.240 plastic 1.650 21.40 24.25 4 130.0869482 0.162 5 3^(rd) lens 8.167310118 0.837 plastic 1.650 21.40 −97.07 6 6.944477468 1.450 7 Aperture plane 0.477 8 4^(th) lens 121.5965254 2.002 plastic 1.565 58.00 9.75 9 −5.755749302 1.515 10 5^(th) lens −86.27705938 4.271 plastic 1.565 58.00 7.16 11 −3.942936258 0.050 12 6^(th) lens 4.867364751 0.300 plastic 1.650 21.40 −6.52 13 2.220604983 0.211 14 7^(th) lens 1.892510651 1.118 plastic 1.650 21.40 8.29 15 2.224128115 1.400 16 Infrared rays plane 0.200 BK_7 1.517 64.2 filter 17 plane 0.917 18 Image plane plane 0 specifically for infrared light Reference wavelength (d-line): 555 nm.

TABLE 2 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k 2.500000E+01 −4.711931E−01 1.531617E+00 −1.153034E+01  −2.915013E+00  4.886991E+00 −3.459463E+01 A4 5.236918E−06 −2.117558E−04 7.146736E−05 4.353586E−04 5.793768E−04 −3.756697E−04  −1.292614E−03 A6 −3.014384E−08  −1.838670E−06 2.334364E−06 1.400287E−05 2.112652E−04 3.901218E−04 −1.602381E−05 A8 −2.487400E−10   9.605910E−09 −7.479362E−08  −1.688929E−07  −1.344586E−05  −4.925422E−05  −8.452359E−06 A10 1.170000E−12 −8.256000E−11 1.701570E−09 3.829807E−08 1.000482E−06 4.139741E−06  7.243999E−07 A12 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 A14 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 Surface 9 10 11 12 13 14 15 k −7.549291E+00 −5.000000E+01  −1.740728E+00  −4.709650E+00 −4.509781E+00 −3.427137E+00 −3.215123E+00  A4 −5.583548E−03 1.240671E−04 6.467538E−04 −1.872317E−03 −8.967310E−04 −3.189453E−03 −2.815022E−03  A6  1.947110E−04 −4.949077E−05  −4.981838E−05  −1.523141E−05 −2.688331E−05 −1.058126E−05 1.884580E−05 A8 −1.486947E−05 2.088854E−06 9.129031E−07 −2.169414E−06 −8.324958E−07  1.760103E−06 −1.017223E−08  A10 −6.501246E−08 −1.438383E−08  7.108550E−09 −2.308304E−08 −6.184250E−09 −4.730294E−08 3.660000E−12 A12  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00 A14  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00

The figures related to the profile curve lengths obtained based on Table 1 and Table 2 are listed in the following table:

First embodiment (Reference wavelength: 555 nm) ARE 1/2(HEP) ARE value ARE − 1/2(HXP) 2(ARE/HXP) % TP ARE/TP (%) 11 1.792 1.792 −0.00044 99.98% 2.276 78.73% 12 1.792 1.806 0.01319 100.74% 2.276 79.33% 21 1.792 1.797 0.00437 100.24% 5.240 34.29% 22 1.792 1.792 −0.00032 99.98% 5.240 34.20% 31 1.792 1.808 0.01525 100.85% 0.837 216.01% 32 1.792 1.819 0.02705 101.51% 0.837 217.42% 41 1.792 1.792 −0.00041 99.98% 2.002 89.50% 42 1.792 1.825 0.03287 101.83% 2.002 91.16% 51 1.792 1.792 −0.00031 99.98% 4.271 41.96% 52 1.792 1.845 0.05305 102.96% 4.271 43.21% 61 1.792 1.818 0.02587 101.44% 0.300 606.10% 62 1.792 1.874 0.08157 104.55% 0.300 624.67% 71 1.792 1.898 0.10523 105.87% 1.118 169.71% 72 1.792 1.885 0.09273 105.17% 1.118 168.59% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP(%) 11 15.095 15.096 0.001 100.01% 2.276 663.24% 12 10.315 11.377 1.062 110.29% 2.276 499.86% 21 7.531 8.696 1.166 115.48% 5.240 165.96% 22 4.759 4.881 0.122 102.56% 5.240 93.15% 31 3.632 4.013 0.382 110.51% 0.837 479.55% 32 2.815 3.159 0.344 112.23% 0.837 377.47% 41 2.967 2.971 0.004 100.13% 2.002 148.38% 42 3.402 3.828 0.426 112.53% 2.002 191.20% 51 4.519 4.523 0.004 100.10% 4.271 105.91% 52 5.016 5.722 0.706 114.08% 4.271 133.99% 61 5.019 5.823 0.805 116.04% 0.300 1941.14% 62 5.629 6.605 0.976 117.34% 0.300 2201.71% 71 5.634 6.503 0.869 115.43% 1.118 581.54% 72 6.488 7.152 0.664 110.24% 1.118 639.59%

The detail parameters of the first embodiment are listed in Table 1, in which the unit of the radius of curvature, thickness, and focal length are millimeter, and surface 0-10 indicates the surfaces of all elements in the system in sequence from the object side to the image side. Table 2 is the list of coefficients of the aspheric surfaces, in which A1-A20 indicate the coefficients of aspheric surfaces from the first order to the twentieth order of each aspheric surface. The following embodiments have the similar diagrams and tables, which are the same as those of the first embodiment, so we do not describe it again.

Second Embodiment

As shown in FIG. 2A and FIG. 2B, an optical image capturing system 20 of the second embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 210, an aperture 200, a second lens 220, a third lens 230, a fourth lens 240, a fifth lens 250, a sixth lens 260, a seven lens 270, an infrared rays filter 280, an image plane specifically for the infrared light 290, and an image sensor 292. FIG. 2C is a transverse aberration diagram at 0.7 field of view of the second embodiment of the present application.

The first lens 210 has positive refractive power and is made of plastic. An object-side surface 212 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 214 thereof, which faces the image side, is a concave aspheric surface, wherein the object-side surface 212 has an inflection point.

The second lens 220 has negative refractive power and is made of plastic. An object-side surface 222 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 224 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 222 has an inflection point, and the image-side surface 224 has an inflection point.

The third lens 230 has positive refractive power and is made of plastic. An object-side surface 232, which faces the object side, is a convex aspheric surface, and an image-side surface 234, which faces the image side, is a concave aspheric surface, wherein the image-side surface 234 has an inflection point.

The fourth lens 240 has positive refractive power and is made of plastic. An object-side surface 242, which faces the object side, is a convex aspheric surface, and an image-side surface 244, which faces the image side, is a concave aspheric surface. The object-side surface 242 has an inflection point, and the image-side surface 244 has an inflection point.

The fifth lens 250 has positive refractive power and is made of plastic. An object-side surface 252, which faces the object side, is a convex aspheric surface, and an image-side surface 254, which faces the image side, is a concave aspheric surface. The object-side surface 252 has an inflection point, and the image-side surface 254 has two inflection points.

The sixth lens 260 has positive refractive power and is made of plastic. An object-side surface 262, which faces the object side, is a convex aspheric surface, and an image-side surface 264, which faces the image side, is a concave aspheric surface. The object-side surface 262 has two inflection points, and the image-side surface 264 has two inflection points. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration.

The seventh lens 270 has negative refractive power and is made of plastic. An object-side surface 272, which faces the object side, is a concave aspheric surface, and an image-side surface 274, which faces the image side, is a concave aspheric surface. The object-side surface 272 has an inflection point, and the image-side surface 274 has an inflection point. It may help to shorten the back focal length to keep small in size, and may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 280 is made of glass and between the seventh lens 270 and the image plane specifically for the infrared light 290. The infrared rays filter 280 gives no contribution to the focal length of the system.

The parameters of the lenses of the second embodiment are listed in Table 3 and Table 4.

TABLE 3 f = 8.6556 mm; f/HEP = 1.4; HAF = 20.5346 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 3.608758597 1.959 plastic 1.544 56.09 8.454 2 13.8060016 0.490 3 Aperture 1E+18 0.150 4 2^(nd) lens −10.34008735 0.400 plastic 1.515 56.55 −9.136 5 8.654799118 0.050 6 3^(rd) lens 4.039776435 0.436 plastic 1.661 20.39 22.206 7 5.362440883 0.050 8 4^(th) lens 2.914317723 0.473 plastic 1.5441 56.090 9091.860 9 2.749936463 0.352 10 5^(th) lens 2.873983403 0.533 plastic 1.661 20.39 13.208 11 3.995948109 1.154 12 6^(th) lens 17.9817901 0.417 plastic 1.661 20.39 100.229 13 24.57331161 1.209 14 7^(th) lens −29.18117929 0.542 plastic 1.636 23.89 −9.731 15 7.792296656 0.171 16 Infrared 1E+18 0.215 BK_7 1.517 64.2 rays filter 17 1E+18 0.999 18 Image plane 1E+18 0.001 specifically for infrared light Reference wavelength: 940 nm; the position of blocking light: the effective half diameter of the clear aperture of the first surface is 3.437 mm; the effective half diameter of the clear aperture of the fifth surface is 2.950 mm; the effective half diameter of the clear aperture of the fifteenth surface is 2.970 mm; in the current embodiment, the first aperture is used for calculating the aperture value, and the exit pupil diameter of the image-side surface of the seventh lens is used as HXP

TABLE 4 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 −6.020435E−01 −3.021045E+00 −3.926596E+01 −2.205177E+01 −1.813067E+00  2.043846E+00 −1.299930E+00  A4 −1.665998E−04 −2.865732E−03 −4.016547E−03 −2.327750E−03  1.086065E−02  1.594973E−02 4.428747E−03 A6  3.563534E−05  8.727019E−04  4.675536E−03  1.503727E−03 −1.841949E−03 −1.722523E−03 5.600680E−05 A8  1.472237E−05 −1.534967E−04 −1.124443E−03 −2.608390E−04 −3.422804E−04 −2.442256E−03 −9.417032E−04  A10 −5.304019E−06  2.881569E−05  1.769086E−04  1.070410E−05  1.340704E−04  9.160450E−04 1.480627E−04 A12  7.575763E−07 −3.136218E−06 −1.779748E−05  8.843343E−07 −1.534288E−05 −1.379784E−04 2.859123E−06 A14 −4.909059E−08  1.537957E−07  1.011806E−06 −5.694768E−08  6.102273E−07  9.285353E−06 −2.687307E−06  A16  1.080216E−09 −2.772807E−09 −2.452775E−08 −4.585678E−10  2.334429E−09 −2.244288E−07 1.820267E−07 Surface 9 10 11 12 13 14 15 k −3.444200E+00  −5.441012E+00  2.299813E−01 −8.999827E+01 −3.396539E+01  8.999091E+01 −2.361751E+01 A4 4.716089E−03 8.913614E−03 −1.707338E−02   1.419255E−03 −5.810072E−03 −4.010619E−02 −3.472495E−02 A6 5.746184E−04 −5.502425E−03  1.850544E−03 −6.280987E−03 −3.099095E−04  8.903957E−03  7.861744E−03 A8 4.056198E−05 3.956161E−04 −1.963177E−03   3.301723E−03  3.772465E−05 −2.222118E−03 −1.724419E−03 A10 −4.277343E−04  2.175856E−04 7.910576E−04 −1.513522E−03 −3.210133E−05  6.986359E−04  3.179609E−04 A12 1.254760E−04 −4.394603E−05  −1.177970E−04   4.042532E−04  1.202548E−05 −1.361232E−04 −3.865119E−05 A14 −1.438544E−05  1.726265E−06 3.472448E−06 −5.898805E−05 −3.410486E−06  1.263136E−05  2.473662E−06 A16 6.053910E−07 6.027942E−08 3.380357E−07  3.479231E−06  3.016620E−07 −4.356463E−07 −6.225282E−08

An equation of the aspheric surfaces of the second embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the second embodiment based on Table 3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 940 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 1.0238 0.9475 0.3898 0.0010 0.6553 0.0864 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.8895 1.5009 2.4923 0.6022 0.0740 0.1397 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.9254 0.4114 6.4988 4.1996 HOS InTL HOS/HOI InS/HOS ODT % TDT % 9.4296 8.2157 2.8574 0.7403 1.7716 1.1496 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0    0    1.4874 0    0    0    HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.7614 0.7282 0    0.8546 0.2590 0.0906 PSTA PLTA NSTA NLTA SSTA SLTA −0.062 mm −0.014 mm −0.007 mm −0.023 mm −0.020 mm −0.002 mm IN12 IN23 IN34 IN45 IN56 IN67 0.6405 mm 0.0500 mm 0.0500 mm 0.3520 mm 1.1540 mm 1.2092 mm

The figures related to the profile curve lengths obtained based on Table 3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 940 nm) ARE 1/2(HXP) ARE value ARE − 1/2(HXP) 2(ARE/HXP) % TP ARE/TP (%) 11 3.210 3.581 0.370 111.53% 1.959 182.78% 12 3.081 3.105 0.024 100.77% 1.959 158.48% 21 2.991 3.066 0.075 102.52% 0.400 766.45% 22 2.950 2.958 0.008 100.26% 0.400 739.39% 31 2.778 2.916 0.138 104.96% 0.436 668.15% 32 2.577 2.706 0.130 105.03% 0.436 620.08% 41 2.482 2.638 0.157 106.32% 0.473 558.22% 42 2.398 2.466 0.069 102.87% 0.473 521.84% 51 2.265 2.315 0.050 102.20% 0.533 434.19% 52 2.153 2.207 0.054 102.49% 0.533 413.93% 61 2.175 2.352 0.177 108.14% 0.417 564.03% 62 2.386 2.510 0.123 105.16% 0.417 601.92% 71 2.651 2.900 0.248 109.37% 0.542 535.22% 72 2.970 3.238 0.268 109.01% 0.542 597.65% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 3.437 3.845 0.408 111.87% 1.959 196.26% 12 3.081 3.105 0.024 100.77% 1.959 158.48% 21 2.991 3.066 0.075 102.52% 0.400 766.45% 22 2.950 2.958 0.008 100.26% 0.400 739.39% 31 2.778 2.916 0.138 104.96% 0.436 668.15% 32 2.577 2.706 0.130 105.03% 0.436 620.08% 41 2.482 2.638 0.157 106.32% 0.473 558.22% 42 2.398 2.466 0.069 102.87% 0.473 521.84% 51 2.265 2.315 0.050 102.20% 0.533 434.19% 52 2.153 2.207 0.054 102.49% 0.533 413.93% 61 2.175 2.352 0.177 108.14% 0.417 564.03% 62 2.386 2.510 0.123 105.16% 0.417 601.92% 71 2.651 2.900 0.248 109.37% 0.542 535.22% 72 2.970 3.238 0.268 109.01% 0.542 597.65%

The results of the equations of the second embodiment based on Table 3 and Table 4 are listed in the following table:

Values related to the inflection points of the second embodiment (Reference wavelength: 940 nm) HIF111 2.7553 HIF111/HOI 0.8349 SGI111 1.0894 |SGI111|/(|SGI111| + TP1) 0.3574 HIF211 0.8718 HIF211/HOI 0.2642 SGI211 −0.0319 |SGI211|/(|SGI211| + TP2) 0.0739 HIF221 2.3452 HIF221/HOI 0.7107 SGI221 0.1573 |SGI221|/(|SGI221| + TP2) 0.2823 HIF321 2.3097 HIF321/HOI 0.6999 SGI321 0.5850 |SGI321|/(|SGI321| + TP3) 0.5727 HIF411 2.1383 HIF411/HOI 0.6480 SGI411 0.6674 |SGI411|/(|SGI411| + TP4) 0.5854 HIF421 1.3945 HIF421/HOI 0.4226 SGI421 0.2998 |SGI421|/(|SGI421| + TP4) 0.3881 HIF511 1.2786 HIF511/HOI 0.3875 SGI511 0.2374 |SGI511|/(|SGI511| + TP5) 0.3081 HIF521 1.4821 HIF521/HOI 0.4491 SGI521 0.2273 |SGI521|/(|SGI521| + TP5) 0.2989 HIF522 1.7387 HIF522/HOI 0.5269 SGI522 0.2907 |SGI522|/(|SGI522| + TP5) 0.3529 HIF611 0.4426 HIF611/HOI 0.1341 SGI611 0.0046 |SGI611|/(|SGI611| + TP6) 0.0109 HIF612 2.1144 HIF612/HOI 0.6407 SGI612 −0.4722 |SGI612|/(|SGI612| + TP6) 0.5311 HIF621 0.4180 HIF621/HOI 0.1267 SGI621 0.0030 |SGI621|/(|SGI621| + TP6) 0.0071 HIF622 2.2740 HIF622/HOI 0.6891 SGI622 −0.3952 |SGI622|/(|SGI622| + TP6) 0.4866 HIF711 2.5009 HIF711/HOI 0.7578 SGI711 −0.7984 |SGI711|/(|SGI711| + TP7) 0.5957 HIF721 0.4574 HIF721/HOI 0.1386 SGI721 0.0110 |SGI721|/(|SGI721| + TP7) 0.0198

Third Embodiment

As shown in FIG. 3A and FIG. 3B, an optical image capturing system 30 of the third embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 310, an aperture 300, a second lens 320, a third lens 330, a fourth lens 340, a fifth lens 350, a sixth lens 360, a seventh lens 370, an infrared rays filter 380, an image plane specifically for the infrared light 390, and an image sensor 392. FIG. 3C is a transverse aberration diagram at 0.7 field of view of the third embodiment of the present application.

The first lens 310 has positive refractive power and is made of plastic. An object-side surface 312 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 314 thereof, which faces the image side, is a concave aspheric surface, wherein the object-side surface 312 has an inflection point, and the image-side surface 314 has an inflection point.

The second lens 320 has negative refractive power and is made of plastic. An object-side surface 322 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 324 thereof, which faces the image side, is a concave aspheric surface, wherein the object-side surface 322 has two inflection points, and the image-side surface 324 has an inflection point.

The third lens 330 has positive refractive power and is made of plastic. An object-side surface 332 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 334 thereof, which faces the image side, is a concave aspheric surface.

The fourth lens 340 has negative refractive power and is made of plastic. An object-side surface 342, which faces the object side, is a convex aspheric surface, and an image-side surface 344, which faces the image side, is a concave aspheric surface, wherein the object-side surface 342 has two inflection points, and the image-side surface 344 has an inflection point.

The fifth lens 350 has positive refractive power and is made of plastic. An object-side surface 352, which faces the object side, is a convex aspheric surface, and an image-side surface 354, which faces the image side, is a concave aspheric surface, wherein the object-side surface 352 has three inflection points, and the image-side surface 354 has two inflection points.

The sixth lens 360 has positive refractive power and is made of plastic. An object-side surface 362, which faces the object side, is a convex aspheric surface, and an image-side surface 364, which faces the image side, is a convex aspheric surface, wherein the object-side surface 362 has two inflection points, and the image-side surface 364 has an inflection point. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration.

The seventh lens 370 has negative refractive power and is made of plastic. An object-side surface 372, which faces the object side, is a convex aspheric surface, and an image-side surface 374, which faces the image side, is a concave aspheric surface. It may help to shorten the back focal length to keep small in size. In addition, the object-side surface 372 has two inflection points, and the image-side surface 374 has an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 380 is made of glass and between the seventh lens 370 and the image plane specifically for the infrared light 390. The infrared rays filter 380 gives no contribution to the focal length of the system.

The parameters of the lenses of the third embodiment are listed in Table 5 and Table 6.

TABLE 5 f = 8.6158 mm; f/HEP = 1.0; HAF = 20.5502 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 5.112456695 2.000 plastic 1.544 56.09 11.506 2 24.59945941 0.346 3 Aperture 1E+18 0.150 4 2^(nd) lens −12.29966691 0.419 plastic 1.515 56.55 −9.682 5 8.401305303 0.050 6 3^(rd) lens 3.380404133 1.347 plastic 1.661 20.39 10.088 7 5.855969919 0.431 8 4^(th) lens 2.7783257 0.543 plastic 1.544 56.09 −191.577 9 2.519978139 1.142 10 5^(th) lens 3.788193622 0.589 plastic 1.661 20.39 15.450 11 5.695684242 1.349 12 6^(th) lens 45.78926584 0.559 plastic 1.661 20.39 54.188 13 −154.4855046 0.230 14 7^(th) lens 4.700764222 0.394 plastic 1.636 23.89 −10.905 15 2.698147892 0.239 16 Infrared 1E+18 0.215 BK_7 1.517 64.2 rays filter 17 1E+18 0.999 18 Image plane 1E+18 0.001 specifically for infrared light Reference wavelength: 940 nm; the position of blocking light: the effective half diameter of the clear aperture of the fourth surface is 4.465 mm; the effective half diameter of the clear aperture of the fifth surface is 4.465 mm; the effective half diameter of the clear aperture of the ninth surface is 3.100 mm; the exit pupil diameter of the image-side surface of the seventh lens is used as HXP

TABLE 6 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −8.274930E−01 −2.567073E+01 −2.693232E+01 −2.822341E+00 −1.506280E+00  1.723385E+00 −1.229266E+00 A4 −5.472769E−04 −2.776560E−03  1.509562E−02  2.097049E−02  8.419929E−03  7.815428E−03 −3.376133E−03 A6  8.353616E−05  1.067811E−03 −2.074464E−03 −5.357177E−03 −2.037358E−03 −1.131033E−03  8.600724E−04 A8 −1.765267E−05 −1.776985E−04  1.840679E−04  5.811635E−04  3.306483E−04 −1.530358E−05 −4.592307E−04 A10  1.850435E−06  1.538122E−05 −1.186089E−05 −3.466600E−05 −5.206337E−05 −5.932071E−06  4.425298E−05 A12 −1.504192E−07 −7.429141E−07  6.368232E−07  1.172483E−06  5.742477E−06  3.389440E−06  1.538306E−06 A14  6.015457E−09  1.898004E−08 −2.219552E−08 −2.123347E−08 −3.343524E−07 −3.639285E−07 −4.269123E−07 A16 −8.820639E−11 −2.015608E−10  3.182121E−10  1.630629E−10  7.739030E−09  1.210206E−08  1.699109E−08 Surface 9 10 11 12 13 14 15 k −3.170098E+00 −7.290405E+00  4.256323E−01 −7.269228E+01 −3.156745E+01 −3.417011E+01 −1.398615E+01 A4  2.106319E−03  3.884817E−03 −1.052475E−02  1.455030E−02 −2.140274E−02 −1.349309E−01 −7.874989E−02 A6  1.472733E−03 −1.384577E−04  2.067012E−03 −2.247441E−02  5.048437E−03  5.903182E−02  3.133721E−02 A8 −9.134375E−04 −1.498622E−03 −1.797602E−03  1.365764E−02  2.037305E−03 −1.392772E−02 −7.652589E−03 A10  1.709433E−04  6.267565E−04  6.188574E−04 −5.233465E−03 −1.529550E−03  1.866830E−03  1.132295E−03 A12 −1.749428E−05 −1.281974E−04 −1.107698E−04  1.091974E−03  3.350093E−04 −1.454527E−04 −1.002298E−04 A14  9.481144E−07  1.283923E−05  9.987438E−06 −1.155219E−04 −3.278021E−05  6.348745E−06  4.896584E−06 A16 −2.050334E−08 −4.921486E−07 −3.343660E−07  4.839359E−06  1.227615E−06 −1.234321E−07 −1.019593E−07

An equation of the aspheric surfaces of the third embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the third embodiment based on Table 5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 940 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.7488 0.8899 0.8541 0.0450 0.5576 0.1590 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.7901 1.8069 2.2376 0.8075 0.0576 0.0267 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 1.1884 0.9598 5.9590 1.1168 HOS InTL HOS/HOI InS/HOS ODT % TDT % 10.8072  9.5482 3.2749 0.7829 2.1571 1.1847 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0    3.9133 1.2870 0    0    0    HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 1.1503 0    0.6371 1.1627 0.3523 0.1076 PSTA PLTA NSTA NLTA SSTA SLTA −0.039 mm  0.008 mm  0.022 mm −0.006 mm −0.038 mm  0.008 mm IN12 IN23 IN34 IN45 IN56 IN67 0.4963 mm 0.0500 mm 0.4306 mm 1.1416 mm 1.3492 mm 0.2301 mm

The figures related to the profile curve lengths obtained based on Table 5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 940 nm) ARE 1/2(HXP) ARE value ARE − 1/2(HXP) 2(ARE/HXP) % TP ARE/TP (%) 11 4.489 4.749 0.260 105.79% 2.000 237.46% 12 4.489 4.498 0.008 100.19% 2.000 224.90% 21 4.465 4.660 0.194 104.35% 0.419 1112.40% 22 4.465 4.545 0.079 101.77% 0.419 1084.89% 31 3.780 4.430 0.651 117.21% 1.347 328.98% 32 3.386 3.667 0.281 108.31% 1.347 272.33% 41 3.258 3.444 0.186 105.71% 0.543 633.91% 42 3.100 3.265 0.165 105.32% 0.543 600.87% 51 2.806 2.850 0.043 101.54% 0.589 483.72% 52 2.705 2.728 0.023 100.85% 0.589 463.09% 61 2.718 3.137 0.418 115.40% 0.559 561.45% 62 2.911 3.267 0.356 112.24% 0.559 584.79% 71 3.021 3.232 0.211 106.97% 0.394 820.72% 72 3.250 3.452 0.203 106.24% 0.394 876.73% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 4.689 4.949 0.260 105.55% 2.000 247.45% 12 4.559 4.569 0.010 100.22% 2.000 228.43% 21 4.465 4.660 0.194 104.35% 0.419 1112.40% 22 4.465 4.545 0.079 101.77% 0.419 1084.89% 31 3.780 4.430 0.651 117.21% 1.347 328.98% 32 3.386 3.667 0.281 108.31% 1.347 272.33% 41 3.258 3.444 0.186 105.71% 0.543 633.91% 42 3.100 3.265 0.165 105.32% 0.543 600.87% 51 2.806 2.850 0.043 101.54% 0.589 483.72% 52 2.705 2.728 0.023 100.85% 0.589 463.09% 61 2.718 3.137 0.418 115.40% 0.559 561.45% 62 2.911 3.267 0.356 112.24% 0.559 584.79% 71 3.021 3.232 0.211 106.97% 0.394 820.72% 72 3.250 3.452 0.203 106.24% 0.394 876.73%

The results of the equations of the third embodiment based on Table 5 and Table 6 are listed in the following table:

Values related to the inflection points of the third embodiment (Reference wavelength: 940 nm) HIF111 3.1047 HIF111/HOI 0.9408 SGI111 0.9030 |SGI111|/(|SGI111| + TP1) 0.3111 HIF121 2.5770 HIF121/HOI 0.7809 SGI121 0.1166 |SGI121|/(|SGI121| + TP1) 0.0551 HIF211 0.6855 HIF211/HOI 0.2077 SGI211 −0.0156 |SGI211|/(|SGI211| + TP2) 0.0359 HIF212 4.0370 HIF212/HOI 1.2233 SGI212 0.6671 |SGI212|/(|SGI212| + TP2) 0.6143 HIF221 1.9144 HIF221/HOI 0.5801 SGI221 0.3157 |SGI221|/(|SGI221| + TP2) 0.4298 HIF411 1.8240 HIF411/HOI 0.5527 SGI411 0.5411 |SGI411|/(|SGI411| + TP4) 0.4990 HIF412 3.1784 HIF412/HOI 0.9631 SGI412 1.0084 |SGI412|/(|SGI412| + TP4) 0.6498 HIF421 1.7809 HIF421/HOI 0.5397 SGI421 0.5307 |SGI421|/(|SGI421| + TP4) 0.4941 HIF511 1.4214 HIF511/HOI 0.4307 SGI511 0.2285 |SGI511|/(|SGI511| + TP5) 0.2795 HIF512 2.6242 HIF512/HOI 0.7952 SGI512 0.3486 |SGI512|/(|SGI512| + TP5) 0.3717 HIF513 2.7118 HIF513/HOI 0.8218 SGI513 0.3353 |SGI513|/(|SGI513| + TP5) 0.3627 HIF521 1.2111 HIF521/HOI 0.3670 SGI521 0.1097 |SGI521|/(|SGI521| + TP5) 0.1570 HIF522 2.2993 HIF522/HOI 0.6968 SGI522 0.1878 |SGI522|/(|SGI522| + TP5) 0.2418 HIF611 0.7630 HIF611/HOI 0.2312 SGI611 0.0081 |SGI611|/(|SGI611| + TP6) 0.0143 HIF612 2.5897 HIF612/HOI 0.7848 SGI612 −0.7611 |SGI612|/(|SGI612| + TP6) 0.5767 HIF621 2.7384 HIF621/HOI 0.8298 SGI621 −0.7906 |SGI621|/(|SGI621| + TP6) 0.5859 HIF711 0.3426 HIF711/HOI 0.1038 SGI711 0.0102 |SGI711|/(|SGI711| + TP7) 0.0253 HIF712 2.5914 HIF712/HOI 0.7853 SGI712 −0.6472 |SGI712|/(|SGI712| + TP7) 0.6217 HIF721 0.5314 HIF721/HOI 0.1610 SGI721 0.0414 |SGI721|/(|SGI721| + TP7) 0.0951

Fourth Embodiment

As shown in FIG. 4A and FIG. 4B, an optical image capturing system 40 of the fourth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 410, an aperture 400, a second lens 420, a third lens 430, a fourth lens 440, a fifth lens 450, a sixth lens 460, a seventh lens 470, an infrared rays filter 480, an image plane specifically for the infrared light 490, and an image sensor 492. FIG. 4C is a transverse aberration diagram at 0.7 field of view of the fourth embodiment of the present application.

The first lens 410 has positive refractive power and is made of plastic. An object-side surface 412 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 414 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 412 has an inflection point.

The second lens 420 has negative refractive power and is made of plastic. An object-side surface 422 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 424 thereof, which faces the image side, is a concave aspheric surface. The image-side surface 424 has an inflection point.

The third lens 430 has positive refractive power and is made of plastic. An object-side surface 432 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 434 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 432 has two inflection points, and the image-side surface 434 has three inflection points.

The fourth lens 440 has positive refractive power and is made of plastic. An object-side surface 442, which faces the object side, is a convex aspheric surface, and an image-side surface 444, which faces the image side, is a concave aspheric surface. The object-side surface 442 has two inflection points, and the image-side surface 444 has two inflection points.

The fifth lens 450 has positive refractive power and is made of plastic. An object-side surface 452, which faces the object side, is a convex aspheric surface, and an image-side surface 454, which faces the image side, is a concave aspheric surface. The object-side surface 452 has an inflection point, and the image-side surface 454 has an inflection point.

The sixth lens 460 has positive refractive power and is made of plastic. An object-side surface 462, which faces the object side, is a convex aspheric surface, and an image-side surface 464, which faces the image side, is a convex aspheric surface. The object-side surface 462 has an inflection point, and the image-side surface 464 has an inflection point. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration.

The seventh lens 470 has negative refractive power and is made of plastic. An object-side surface 472, which faces the object side, is a convex aspheric surface, and an image-side surface 474, which faces the image side, is a concave aspheric surface. The object-side surface 472 has two inflection points, and the image-side surface 474 has two inflection points. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 480 is made of glass and between the seventh lens 470 and the image plane specifically for the infrared light 490. The infrared rays filter 480 gives no contribution to the focal length of the system.

The parameters of the lenses of the fourth embodiment are listed in Table 7 and Table 8.

f = 6.7787 mm; f/HEP = 1.4; HAF = 25.6275 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 3.422929224 0.696 plastic 1.584 29.89 19.272 2 4.57054616 0.846 3 Aperture 1E+18 −0.321  4 2^(nd) lens 22.29252636 0.738 plastic 1.515 56.55 −35.085 5 9.836765156 0.150 6 3^(rd) lens 22.8180854 0.543 plastic 1.661 20.39 111.489 7 32.93339546 0.050 8 4^(th) lens 2.368073586 0.978 plastic 1.544 56.09 21.288 9 2.547918656 0.228 10 5^(th) lens 2.560253873 0.602 plastic 1.661 20.39 13.392 11 3.284885133 1.203 12 6^(th) lens 19.58525893 0.727 plastic 1.661 20.39 9.242 13 −8.586539162 0.758 14 7^(th) lens 29.10157108 0.359 plastic 1.636 23.89 −5.979 15 3.312112442 0.228 16 Infrared 1E+18 0.215 BK_7 1.517 64.2 rays filter 17 1E+18 1.000 18 Image plane 1E+18 0.000 specifically for infrared light Reference wavelength: 940 nm; the position of blocking light: the effective half diameter of the clear aperture of the sixth surface is 2.746 mm; the effective half diameter of the clear aperture of the seventh surface is 2.770 mm; the effective half diameter of the clear aperture of the fifteenth surface is 2.950 mm; the exit pupil diameter of the image-side surface of the seventh lens is used as HXP

TABLE 8 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −2.319837E+00 −9.200961E+00 6.852471E+01 −8.945487E+01 6.503287E+01 8.988503E+01 −1.212746E+00 A4  3.754323E−03  1.273511E−02 1.395197E−02  1.788787E−02 6.017742E−03 5.627701E−03 −7.360646E−04 A6 −1.816684E−03 −6.074251E−03 −9.687121E−03  −1.849369E−02 −3.743121E−03  −2.242977E−03  −2.492451E−03 A8  3.151676E−04  1.128158E−03 3.357512E−03  7.075838E−03 1.191534E−04 2.946467E−04  5.238502E−04 A10 −9.255319E−05 −1.091122E−04 −5.754096E−04  −1.482386E−03 3.004769E−04 7.993898E−06  9.690364E−05 A12  1.427989E−05  1.405535E−05 6.353942E−05  1.865340E−04 −8.628215E−05  −1.100013E−05  −8.752066E−05 A14 −8.699769E−07 −2.283839E−06 −5.080905E−06  −1.397226E−05 9.987259E−06 2.012662E−06  1.713495E−05 A16  1.727348E−08  1.565328E−07 2.010750E−07  4.914979E−07 −4.295077E−07  −1.254936E−07  −1.076750E−06 Surface 9 10 11 12 13 14 15 k −6.934912E+00 −6.306659E+00  2.138094E−01 −8.998695E+01 −2.749949E+01  8.900696E+01 −1.427832E+01 A4  6.565919E−03  1.977947E−03 −1.376303E−02 −3.332985E−03 −8.580272E−03 −1.087960E−01 −6.615250E−02 A6 −3.199442E−03 −1.176738E−03  5.012094E−03 −1.448698E−03  1.930532E−03  4.370249E−02  2.569579E−02 A8 −2.316685E−03 −2.220488E−03 −2.380857E−03  3.294246E−04 −2.070344E−04 −1.150533E−02 −6.706569E−03 A10  1.287927E−03  1.517894E−03  1.422015E−03  5.389812E−07 −8.202646E−07  2.030953E−03  1.138817E−03 A12 −2.686568E−04 −3.501910E−04 −3.495731E−04 −1.751515E−05  2.236784E−05 −2.179917E−04 −1.211066E−04 A14  2.893757E−05  3.727091E−05  3.396473E−05  2.739816E−06 −6.292785E−06  1.281568E−05  7.307362E−06 A16 −1.344272E−06 −1.680183E−06 −1.190062E−06 −3.335559E−07  4.770092E−07 −3.191279E−07 −1.887382E−07

An equation of the aspheric surfaces of the fourth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the fourth embodiment based on Table 7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 940 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.3517 0.1932 0.0608 0.3184 0.5062 0.7334 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 1.1337 1.4644 1.8331 0.7989 0.0774 0.1118 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.5493 0.3147 1.6544 1.5370 HOS InTL HOS/HOI InS/HOS ODT % TDT % 8.8584 7.5569 2.6844 0.8259 1.4828 0.5507 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0    0    0    2.1143 0    0    HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 1.3795 0    0.2888 1.2077 0.3660 0.1363 PSTA PLTA NSTA NLTA SSTA SLTA −0.017 mm  0.003 mm  0.021 mm  0.010 mm −0.013 mm −0.001 mm IN12 IN23 IN34 IN45 IN56 IN67 0.5246 mm 0.1500 mm 0.0500 mm 0.2283 mm 1.2028 mm 0.7580 mm

The figures related to the profile curve lengths obtained based on Table 7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 940 nm) ARE 1/2(HXP) ARE value ARE − 1/2(HXP) 2(ARE/HXP) % TP ARE/TP (%) 11 2.509 2.610 0.101 104.04% 0.696 374.86% 12 2.509 2.576 0.067 102.68% 0.696 369.97% 21 2.509 2.567 0.058 102.33% 0.738 347.87% 22 2.509 2.512 0.003 100.12% 0.738 340.38% 31 2.509 2.515 0.006 100.22% 0.543 463.47% 32 2.509 2.512 0.003 100.13% 0.543 463.03% 41 2.482 2.704 0.222 108.94% 0.978 276.39% 42 2.393 2.454 0.061 102.53% 0.978 250.76% 51 2.353 2.472 0.119 105.06% 0.602 410.41% 52 2.218 2.445 0.227 110.22% 0.602 406.05% 61 2.243 2.280 0.037 101.64% 0.727 313.76% 62 2.460 2.489 0.029 101.18% 0.727 342.47% 71 2.509 2.611 0.102 104.05% 0.359 727.37% 72 2.509 2.538 0.029 101.14% 0.359 707.03% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 2.815 2.929 0.114 104.05% 0.696 420.59% 12 2.586 2.664 0.077 103.00% 0.696 382.53% 21 2.525 2.586 0.060 102.39% 0.738 350.34% 22 2.555 2.557 0.003 100.11% 0.738 346.49% 31 2.746 2.763 0.018 100.65% 0.543 509.34% 32 2.770 2.776 0.005 100.19% 0.543 511.58% 41 2.482 2.704 0.222 108.94% 0.978 276.39% 42 2.393 2.454 0.061 102.53% 0.978 250.76% 51 2.353 2.472 0.119 105.06% 0.602 410.41% 52 2.218 2.445 0.227 110.22% 0.602 406.05% 61 2.243 2.280 0.037 101.64% 0.727 313.76% 62 2.460 2.489 0.029 101.18% 0.727 342.47% 71 2.752 2.853 0.101 103.68% 0.359 794.95% 72 2.950 3.003 0.053 101.81% 0.359 836.84%

The results of the equations of the fourth embodiment based on Table 7 and Table 8 are listed in the following table:

Values related to the inflection points of the fourth embodiment (Reference wavelength: 940 nm) HIF111 1.7103 HIF111/HOI 0.5183 SGI111 0.3943 |SGI111|/(|SGI111| + TP1) 0.3615 HIF112 2.5197 HIF112/HOI 0.7635 SGI112 0.6659 |SGI112|/(|SGI112| + TP1) 0.4888 HIF221 0.9477 HIF221/HOI 0.2872 SGI221 0.0437 |SGI221|/(|SGI221| + TP2) 0.0559 HIF311 1.2856 HIF311/HOI 0.3896 SGI311 0.0410 |SGI311|/(|SGI311| + TP3) 0.0703 HIF312 1.7426 HIF312/HOI 0.5281 SGI312 0.0660 |SGI312|/(|SGI312| + TP3) 0.1085 HIF321 1.6634 HIF321/HOI 0.5040 SGI321 0.0560 |SGI321|/(|SGI321| + TP3) 0.0936 HIF322 1.9304 HIF322/HOI 0.5850 SGI322 0.0725 |SGI322|/(|SGI322| + TP3) 0.1178 HIF323 2.4141 HIF323/HOI 0.7315 SGI323 0.1055 |SGI323|/(|SGI323| + TP3) 0.1629 HIF411 1.8227 HIF411/HOI 0.5523 SGI411 0.6271 |SGI411|/(|SGI411| + TP4) 0.3906 HIF421 1.1389 HIF421/HOI 0.3451 SGI421 0.2065 |SGI421|/(|SGI421| + TP4) 0.1743 HIF422 1.9022 HIF422/HOI 0.5764 SGI422 0.3904 |SGI422|/(|SGI422| + TP4) 0.2852 HIF511 2.1362 HIF511/HOI 0.6473 SGI511 0.5906 |SGI511|/(|SGI511| + TP5) 0.4951 HIF521 2.0161 HIF521/HOI 0.6110 SGI521 0.7070 |SGI521|/(|SGI521| + TP5) 0.5400 HIF611 0.8192 HIF611/HOI 0.2482 SGI611 0.0146 |SGI611|/(|SGI611| + TP6) 0.0197 HIF621 2.4022 HIF621/HOI 0.7280 SGI621 −0.3221 |SGI621|/(|SGI621| + TP6) 0.3071 HIF711 0.1649 HIF711/HOI 0.0500 SGI711 0.0004 |SGI711|/(|SGI711| + TP7) 0.0011 HIF712 1.8319 HIF712/HOI 0.5551 SGI712 −0.3594 |SGI712|/(|SGI712| + TP7) 0.5004 HIF721 0.5635 HIF721/HOI 0.1708 SGI721 0.0381 |SGI721|/(|SGI721| + TP7) 0.0960 HIF722 2.6593 HIF722/HOI 0.8058 SGI722 −0.1949 |SGI722|/(|SGI722| + TP7) 0.3520

Fifth Embodiment

As shown in FIG. 5A and FIG. 5B, an optical image capturing system 50 of the fifth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 510, an aperture 500, a second lens 520, a third lens 530, a fourth lens 540, a fifth lens 550, a sixth lens 560, a seventh lens 570, an infrared rays filter 580, an image plane specifically for the infrared light 590, and an image sensor 592. FIG. 5C is a transverse aberration diagram at 0.7 field of view of the fifth embodiment of the present application.

The first lens 510 has positive refractive power and is made of plastic. An object-side surface 512, which faces the object side, is a convex aspheric surface, and an image-side surface 514, which faces the image side, is a concave aspheric surface. The object-side surface 512 has two inflection points, and the image-side surface 514 has three inflection points.

The second lens 520 has negative refractive power and is made of plastic. An object-side surface 522 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 524 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 522 has an inflection point, and the image-side surface 524 has three inflection points.

The third lens 530 has negative refractive power and is made of plastic. An object-side surface 532, which faces the object side, is a concave aspheric surface, and an image-side surface 534, which faces the image side, is a convex aspheric surface. The object-side surface 532 has an inflection point, and the image-side surface 534 has two inflection points.

The fourth lens 540 has negative refractive power and is made of plastic. An object-side surface 542, which faces the object side, is a convex aspheric surface, and an image-side surface 544, which faces the image side, is a concave aspheric surface. The object-side surface 542 has an inflection point, and the image-side surface 544 has three inflection points.

The fifth lens 550 has positive refractive power and is made of plastic. An object-side surface 552, which faces the object side, is a convex aspheric surface, and an image-side surface 554, which faces the image side, is a concave aspheric surface. The object-side surface 552 has an inflection point, and the image-side surface 554 has an inflection point.

The sixth lens 560 has positive refractive power and is made of plastic. An object-side surface 562, which faces the object side, is a convex aspheric surface, and an image-side surface 564, which faces the image side, is a convex aspheric surface. The object-side surface 562 has an inflection point, and the image-side surface 564 has two inflection points. Whereby, incident angle of each field of view for the sixth lens 560 can be effectively adjusted to improve aberration.

The seventh lens 570 has negative refractive power and is made of plastic. An object-side surface 572, which faces the object side, is a concave aspheric surface, and an image-side surface 574, which faces the image side, is a concave aspheric surface. The object-side surface 572 has an inflection point, and the image-side surface 574 has two inflection points. It may help to shorten the back focal length to keep small in size. In addition, it may help to shorten the back focal length to keep small in size. In addition, it could effectively suppress the incidence angle of light in the off-axis view field, and correct the off-axis view field aberration.

The infrared rays filter 580 is made of glass and between the seventh lens 570 and the image plane specifically for the infrared light 590. The infrared rays filter 580 gives no contribution to the focal length of the system.

The parameters of the lenses of the fifth embodiment are listed in Table 9 and Table 10.

TABLE 9 f = 6.7546 mm; f/HEP = 1.0; HAF = 25.7508 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 5.298245424 0.803 plastic 1.584 29.89 11.921 2 21.57523391 1.000 3 Aperture 1E+18 −0.697  4 2^(nd) lens 23.40585276 1.040 plastic 1.515 56.55 −95.106 5 15.57045994 0.881 6 3^(rd) lens −2.992855613 0.664 plastic 1.661 20.39 −104.018 7 −3.405383503 0.050 8 4^(th) lens 2.574574018 0.628 plastic 1.544 56.09 −29.561 9 2.027728857 0.064 10 5^(th) lens 2.123128122 0.769 plastic 1.661 20.39 8.130 11 3.033309022 1.437 12 6^(th) lens 22.79085785 0.793 plastic 1.661 20.39 9.104 13 −7.9244487 0.687 14 7^(th) lens −30.54121414 0.350 plastic 1.636 23.89 −7.193 15 5.32930708 0.215 16 Infrared 1E+18 0.215 BK_7 1.517 64.2 rays filter 17 1E+18 0.999 18 Image plane 1E+18 0.000 specifically for infrared light Reference wavelength: 940 nm; the position of blocking light: the effective half diameter of the clear aperture of the first surface is 3.850 mm; the effective half diameter of the clear aperture of the sixth surface is 3.468 mm; the effective half diameter of the clear aperture of the seventh surface is 3.468 mm; the effective half diameter of the clear aperture of the fifteenth surface is 3.220 mm; the exit pupil diameter of the image-side surface of the seventh lens is used as HXP

TABLE 10 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −5.245636E+00 −8.053831E+01 3.783436E+01 −8.999849E+01 −1.073550E+01 −1.270020E+01 −1.088205E+00 A4  1.928599E−03  4.942448E−03 8.338823E−03  3.456488E−03 −3.712552E−03 −9.643133E−03 −1.835446E−02 A6 −7.897549E−04 −2.857701E−03 −3.761874E−03  −3.046736E−03  1.016865E−03  3.333087E−03  4.894732E−03 A8  2.638472E−05  7.173579E−04 1.181456E−03  9.194580E−04 −7.610935E−05 −6.447460E−04 −1.365563E−03 A10 −3.719980E−06 −1.008558E−04 −1.824933E−04  −1.645991E−04 −1.441722E−06  9.187533E−05  2.596052E−04 A12  7.864408E−07  7.947799E−06 1.524817E−05  1.721252E−05  1.140757E−06 −8.327670E−06 −2.908487E−05 A14 −5.082501E−08 −3.254641E−07 −6.731053E−07  −9.315642E−07 −8.523554E−08  4.114781E−07  1.900000E−06 A16  1.061118E−09  5.381534E−09 1.206802E−08  1.987826E−08  1.763176E−09 −8.500219E−09 −5.878333E−08 Surface 9 10 11 12 13 14 15 k −4.861370E+00 −3.151498E+00 −1.380852E−01 −8.999002E+01 −3.395831E+01  8.997881E+01 −1.540630E+01 A4  1.847371E−02  1.578337E−02 −2.802058E−03  1.765631E−03 −6.166059E−03 −5.367681E−02 −4.350907E−02 A6 −2.085130E−02 −1.170561E−02  2.986950E−03  4.956375E−04  4.293549E−03  2.087925E−02  1.701734E−02 A8  7.418098E−03  4.139603E−03 −1.100715E−03 −7.708985E−05 −1.164607E−03 −5.302619E−03 −4.505894E−03 A10 −1.415525E−03 −7.914835E−04  1.035897E−04 −1.081823E−05  2.277156E−04  8.425794E−04  7.588408E−04 A12  1.595465E−04  8.848275E−05  1.196524E−05  7.453158E−06 −2.269772E−05 −7.110360E−05 −7.720766E−05 A14 −9.837656E−06 −5.393224E−06 −2.975898E−06 −1.663596E−06  6.409401E−07  2.703230E−06  4.339745E−06 A16  2.496134E−07  1.295827E−07  1.462739E−07  9.358254E−08  1.544011E−08 −2.783714E−08 −1.029223E−07

An equation of the aspheric surfaces of the fifth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the fifth embodiment based on Table 9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 940 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.5666 0.0710 0.0649 0.2285 0.8308 0.7420 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.9391 1.6020 1.8409 0.8702 0.0448 0.1017 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.1253 0.9143 1.0637 1.3078 HOS InTL HOS/HOI InS/HOS ODT % TDT % 9.7349 8.4701 2.9500 0.8148 1.2770 0.5062 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 2.8242 0    0    3.4212 2.8786 0    HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 2.3264 2.0658 2.6379 1.4103 0.4274 0.1449 PSTA PLTA NSTA NLTA SSTA SLTA −0.067 mm −0.017 mm  0.990 mm  0.004 mm −0.041 mm −0.001 mm IN12 IN23 IN34 IN45 IN56 IN67 0.3024 mm 0.8814 mm 0.0500 mm 0.0639 mm 1.4372 mm 0.6872 mm

The figures related to the profile curve lengths obtained based on Table 9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 940 nm) ARE 1/2(HXP) ARE value ARE − 1/2(HXP) 2(ARE/HXP) % TP ARE/TP (%) 11 3.511 3.556 0.045 101.27% 0.803 442.56% 12 3.511 3.513 0.002 100.07% 0.803 437.31% 21 3.511 3.647 0.136 103.87% 1.040 350.80% 22 3.511 3.514 0.003 100.08% 1.040 338.01% 31 3.468 3.553 0.085 102.45% 0.664 534.75% 32 3.468 3.543 0.075 102.15% 0.664 533.23% 41 3.062 3.368 0.305 109.96% 0.628 536.08% 42 2.990 3.154 0.164 105.48% 0.628 502.03% 51 2.875 3.195 0.320 111.13% 0.769 415.35% 52 2.717 3.081 0.364 113.38% 0.769 400.49% 61 2.731 2.779 0.047 101.73% 0.793 350.34% 62 2.972 2.994 0.022 100.72% 0.793 377.44% 71 3.153 3.227 0.074 102.33% 0.350 921.90% 72 3.220 3.230 0.010 100.31% 0.350 922.82% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 3.850 3.902 0.052 101.36% 0.803 485.74% 12 3.742 3.746 0.003 100.08% 0.803 466.21% 21 3.557 3.693 0.136 103.83% 1.040 355.24% 22 3.520 3.523 0.003 100.08% 1.040 338.87% 31 3.468 3.553 0.085 102.45% 0.664 534.75% 32 3.468 3.543 0.075 102.15% 0.664 533.23% 41 3.062 3.368 0.305 109.96% 0.628 536.08% 42 2.990 3.154 0.164 105.48% 0.628 502.03% 51 2.875 3.195 0.320 111.13% 0.769 415.35% 52 2.717 3.081 0.364 113.38% 0.769 400.49% 61 2.731 2.779 0.047 101.73% 0.793 350.34% 62 2.972 2.994 0.022 100.72% 0.793 377.44% 71 3.153 3.227 0.074 102.33% 0.350 921.90% 72 3.220 3.230 0.010 100.31% 0.350 922.82%

The results of the equations of the fifth embodiment based on Table 9 and Table 10 are listed in the following table:

Values related to the inflection points of the fifth embodiment (Reference wavelength: 940 nm) HIF111 1.7198 HIF111/HOI 0.5212 SGI111 0.2515 |SGI111|/(|SGI111| + TP1) 0.2384 HIF112 3.8276 HIF112/HOI 1.1599 SGI112 0.2909 |SGI112|/(|SGI112| + TP1) 0.2658 HIF121 1.6129 HIF121/HOI 0.4887 SGI121 0.0609 |SGI121|/(|SGI121| + TP1) 0.0705 HIF122 3.0770 HIF122/HOI 0.9324 SGI122 0.1294 |SGI122|/(|SGI122| + TP1) 0.1387 HIF123 3.5286 HIF123/HOI 1.0693 SGI123 0.1413 |SGI123|/(|SGI123| + TP1) 0.1496 HIF211 3.0150 HIF211/HOI 0.9136 SGI211 0.5603 |SGI211|/(|SGI211| + TP2) 0.3502 HIF221 1.2598 HIF221/HOI 0.3818 SGI221 0.0461 |SGI221|/(|SGI221| + TP2) 0.0425 HIF222 2.4869 HIF222/HOI 0.7536 SGI222 0.0921 |SGI222|/(|SGI222| + TP2) 0.0814 HIF223 3.1621 HIF223/HOI 0.9582 SGI223 0.1214 |SGI223|/(|SGI223| + TP2) 0.1046 HIF311 1.7161 HIF311/HOI 0.5200 SGI311 −0.3344 |SGI311|/(|SGI311| + TP3) 0.3348 HIF321 1.7553 HIF321/HOI 0.5319 SGI321 −0.3317 |SGI321|/(|SGI321| + TP3) 0.3329 HIF322 3.1435 HIF322/HOI 0.9526 SGI322 −0.6300 |SGI322|/(|SGI322| + TP3) 0.4867 HIF411 2.7914 HIF411/HOI 0.8459 SGI411 1.1052 |SGI411|/(|SGI411| + TP4) 0.6376 HIF421 1.1380 HIF421/HOI 0.3449 SGI421 0.2587 |SGI421|/(|SGI421| + TP4) 0.2917 HIF422 1.8434 HIF422/HOI 0.5586 SGI422 0.4914 |SGI422|/(|SGI422| + TP4) 0.4389 HIF423 2.6897 HIF423/HOI 0.8151 SGI423 0.8243 |SGI423|/(|SGI423| + TP4) 0.5675 HIF511 2.4656 HIF511/HOI 0.7471 SGI511 1.0510 |SGI511|/(|SGI511| + TP5) 0.5774 HIF521 2.3776 HIF521/HOI 0.7205 SGI521 1.0234 |SGI521|/(|SGI521| + TP5) 0.5709 HIF611 1.9504 HIF611/HOI 0.5910 SGI611 0.1086 |SGI611|/(|SGI611| + TP6) 0.1205 HIF621 1.2702 HIF621/HOI 0.3849 SGI621 −0.0901 |SGI621|/(|SGI621| + TP6) 0.1020 HIF622 2.3880 HIF622/HOI 0.7236 SGI622 −0.1403 |SGI622|/(|SGI622| + TP6) 0.1503 HIF711 1.9336 HIF711/HOI 0.5859 SGI711 −0.3155 |SGI711|/(|SGI711| + TP7) 0.4741 HIF721 0.6339 HIF721/HOI 0.1921 SGI721 0.0299 |SGI721|/(|SGI721| + TP7) 0.0788 HIF722 2.5154 HIF722/HOI 0.7623 SGI722 −0.0251 |SGI722|/(|SGI722| + TP7) 0.0669

Sixth Embodiment

As shown in FIG. 6A and FIG. 6B, an optical image capturing system 60 of the sixth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 610, an aperture 600, a second lens 620, a third lens 630, a fourth lens 640, a fifth lens 650, a seventh lens 660, a seventh lens 670, an infrared rays filter 680, an image plane specifically for the infrared light 690, and an image sensor 692. FIG. 6C is a transverse aberration diagram at 0.7 field of view of the sixth embodiment of the present application.

The first lens 610 has positive refractive power and is made of plastic. An object-side surface 612, which faces the object side, is a convex aspheric surface, and an image-side surface 614, which faces the image side, is a concave aspheric surface. The object-side surface 612 and the image-side surface 614 both have two inflection points.

The second lens 620 has negative refractive power and is made of plastic. An object-side surface 622 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 624 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 622 and the image-side surface 624 both have an inflection point.

The third lens 630 has positive refractive power and is made of plastic. An object-side surface 632, which faces the object side, is a convex aspheric surface, and an image-side surface 634, which faces the image side, is a concave aspheric surface. The object-side surface 632 has two inflection points, and the image-side surface 634 has an inflection point.

The fourth lens 640 has positive refractive power and is made of plastic. An object-side surface 642, which faces the object side, is a convex aspheric surface, and an image-side surface 644, which faces the image side, is a concave aspheric surface. The object-side surface 642 has two inflection points, and the image-side surface 644 has two inflection points.

The fifth lens 650 has positive refractive power and is made of plastic. An object-side surface 652, which faces the object side, is a convex aspheric surface, and an image-side surface 654, which faces the image side, is a concave aspheric surface. The object-side surface 652 and the image-side surface 654 both have an inflection point.

The sixth lens 660 has positive refractive power and is made of plastic. An object-side surface 662, which faces the object side, is a concave aspheric surface, and an image-side surface 664, which faces the image side, is a convex aspheric surface. The object-side surface 662 has an inflection point, and the image-side surface 664 has two inflection points. Whereby, incident angle of each field of view for the sixth lens 660 can be effectively adjusted to improve aberration.

The seventh lens 670 has negative refractive power and is made of plastic. An object-side surface 672, which faces the object side, is a convex aspheric surface, and an image-side surface 674, which faces the image side, is a concave aspheric surface. The object-side surface 672 has an inflection point, and the image-side surface 674 has two inflection points. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 680 is made of glass and between the seventh lens 670 and the image plane specifically for the infrared light 690. The infrared rays filter 680 gives no contribution to the focal length of the system.

The parameters of the lenses of the sixth embodiment are listed in Table 11 and Table 12.

TABLE 11 f = 5.4554 mm; f/HEP = 1.0; HAF = 30.7306 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 7.403214857 0.636 plastic 1.661 20.39 16.166 2 23.98518038 0.492 3 Aperture 1E+18 −0.192  4 2^(nd) lens 27.4566196 0.502 plastic 1.535 56.27 −9.745 5 4.332797437 0.141 6 3^(rd) lens 4.806045993 1.216 plastic 1.661 20.39 95.528 7 4.68719334 0.025 8 4^(th) lens 1.919925537 0.404 plastic 1.661 20.39 183.635 9 1.789112884 0.195 10 5^(th) lens 1.629179352 0.794 plastic 1.661 20.39 4.794 11 2.745525008 1.360 12 6^(th) lens −15.5607797 1.103 plastic 1.661 20.39 3.090 13 −1.835123842 0.058 14 7^(th) lens 4.668747528 0.496 plastic 1.636 23.89 −3.411 15 1.408817508 0.555 16 Infrared 1E+18 0.215 BK_7 1.517 64.2 rays filter 17 1E+18 1.000 18 Image plane 1E+18 0.000 specifically for infrared light Reference wavelength: 940 nm; the position of blocking light: the effective half diameter of the clear aperture of the sixth surface is 3.052 mm; the effective half diameter of the clear aperture of the seventh surface is 3.052 mm; the effective half diameter of the clear aperture of the fifteenth surface is 3.100 mm; the exit pupil diameter of the image-side surface of the seventh lens is used as HXP

TABLE 12 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −6.471522E+00 5.017512E+01 8.468561E+01 1.519050E−01 −5.849631E−01 −4.323861E+01 −1.757211E+00 A4 −1.909932E−03 2.464708E−03 6.877273E−03 2.028632E−02  3.324090E−02  3.829457E−02 −3.272666E−02 A6 −2.183382E−03 −1.658762E−03  3.504253E−03 −1.388918E−02 −1.792549E−02 −2.778540E−02  1.959961E−02 A8  3.649789E−04 9.385835E−05 −1.485691E−03  3.750999E−03  4.378395E−03  7.458736E−03 −7.161591E−03 A10 −3.103639E−05 −1.741197E−06  2.773940E−04 −6.050352E−04 −6.921896E−04 −1.152818E−03  1.291453E−03 A12  2.599034E−06 2.546850E−06 −3.323699E−05  5.085651E−05  6.335653E−05  1.062509E−04 −1.204098E−04 A14 −1.795986E−07 −3.539700E−07  2.441048E−06 −1.934188E−06 −2.833287E−06 −5.362706E−06  5.498825E−06 A16  5.397901E−09 1.307455E−08 −9.297826E−08  1.919408E−08  4.355499E−08  1.130535E−07 −9.041571E−08 Surface 9 10 11 12 13 14 15 k −4.449897E+00 −3.257344E+00 −6.344560E−02 −8.949906E+01 −5.814758E+00 −8.463555E+01 −7.439015E+00 A4 −3.315092E−02  8.706007E−03  1.968907E−02  3.833713E−03  1.024842E−02 −8.118480E−03 −2.173600E−02 A6  2.398266E−02 −9.662848E−05 −7.719420E−03  1.775964E−03 −1.218976E−02 −5.344868E−03  5.028822E−03 A8 −5.864643E−03 −1.825622E−03 −1.561896E−03 −2.571649E−03  6.468174E−03  2.793763E−03 −1.216120E−03 A10  5.288627E−04  1.007111E−03  1.266608E−03  1.287524E−03 −1.941318E−03 −6.347361E−04  2.135051E−04 A12  1.421727E−05 −2.261510E−04 −2.744341E−04 −2.919860E−04  3.690127E−04  7.790082E−05 −2.508976E−05 A14 −5.682184E−06  2.391817E−05  2.540394E−05  3.301279E−05 −3.734553E−05 −4.744222E−06  1.663485E−06 A16  2.790551E−07 −1.030034E−06 −9.176693E−07 −1.575743E−06  1.478237E−06  1.090987E−07 −4.480557E−08

An equation of the aspheric surfaces of the sixth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the sixth embodiment based on Table 11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 940 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.3375 0.5598 0.0571 0.0297 1.1379 1.7654 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 1.5996 3.3276 2.1594 1.5410 0.0550 0.0106 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 1.6589 0.1020 1.8638 0.5016 HOS InTL HOS/HOI InS/HOS ODT % TDT % 8.8201 7.2297 2.6727 0.8721 1.7527 0.7735 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 2.0395 1.8794 2.6201 2.4199 2.4397 1.6489 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 1.6216 2.1706 1.2956 2.1187 0.6420 0.2402 PSTA PLTA NSTA NLTA SSTA SLTA −0.020 mm  0.027 mm  0.020 mm −0.019 mm  0.024 mm  0.051 mm IN12 IN23 IN34 IN45 IN56 IN67 0.3001 mm 0.1412 mm 0.0250 mm 0.1946 mm 1.3599 mm 0.0576 mm

The figures related to the profile curve lengths obtained based on Table 11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 940 nm) ARE 1/2(HXP) ARE value ARE − 1/2(HXP) 2(ARE/HXP) % TP ARE/TP (%) 11 2.845 2.854 0.009 100.30% 0.636 448.69% 12 2.845 2.848 0.003 100.11% 0.636 447.81% 21 2.845 2.906 0.061 102.14% 0.502 578.59% 22 2.845 2.942 0.097 103.42% 0.502 585.83% 31 2.845 2.910 0.065 102.29% 1.216 239.29% 32 2.845 2.912 0.067 102.34% 1.216 239.41% 41 2.845 3.026 0.181 106.36% 0.404 749.24% 42 2.801 3.018 0.216 107.73% 0.404 747.22% 51 2.645 2.996 0.351 113.29% 0.794 377.39% 52 2.628 2.913 0.284 110.82% 0.794 366.91% 61 2.552 2.568 0.016 100.62% 1.103 232.71% 62 2.698 2.797 0.099 103.67% 1.103 253.53% 71 2.845 2.856 0.011 100.37% 0.496 575.84% 72 2.845 2.908 0.063 102.20% 0.496 586.34% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 3.569 3.586 0.018 100.49% 0.636 563.84% 12 3.288 3.291 0.004 100.11% 0.636 517.50% 21 2.873 2.943 0.070 102.45% 0.502 585.97% 22 3.036 3.207 0.171 105.64% 0.502 638.53% 31 3.052 3.117 0.065 102.13% 1.216 256.28% 32 3.052 3.142 0.090 102.96% 1.216 258.37% 41 2.929 3.122 0.193 106.60% 0.404 773.12% 42 2.801 3.018 0.216 107.73% 0.404 747.22% 51 2.645 2.996 0.351 113.29% 0.794 377.39% 52 2.628 2.913 0.284 110.82% 0.794 366.91% 61 2.552 2.568 0.016 100.62% 1.103 232.71% 62 2.698 2.797 0.099 103.67% 1.103 253.53% 71 2.951 2.962 0.011 100.39% 0.496 597.31% 72 3.100 3.179 0.079 102.56% 0.496 641.14%

The results of the equations of the sixth embodiment based on Table 11 and Table 12 are listed in the following table:

Values related to the inflection points of the sixth embodiment (Reference wavelength: 940 nm) HIF111 1.1749 HIF111/HOI 0.3560 SGI111 0.0820 |SGI111|/(|SGI111| + TP1) 0.1142 HIF112 2.6747 HIF112/HOI 0.8105 SGI112 0.1089 |SGI112|/(|SGI112| + TP1) 0.1462 HIF121 1.2408 HIF121/HOI 0.3760 SGI121 0.0336 |SGI121|/(|SGI121| + TP1) 0.0502 HIF122 2.5783 HIF122/HOI 0.7813 SGI122 0.0180 |SGI122|/(|SGI122| + TP1) 0.0275 HIF211 2.1407 HIF211/HOI 0.6487 SGI211 0.2634 |SGI211|/(|SGI211| + TP2) 0.3440 HIF221 1.6341 HIF221/HOI 0.4952 SGI221 0.3273 |SGI221|/(|SGI221| + TP2) 0.3946 HIF311 1.5162 HIF311/HOI 0.4595 SGI311 0.2859 |SGI311|/(|SGI311| + TP3) 0.1903 HIF312 2.7512 HIF312/HOI 0.8337 SGI312 0.4723 |SGI312|/(|SGI312| + TP3) 0.2797 HIF321 0.9937 HIF321/HOI 0.3011 SGI321 0.0946 |SGI321|/(|SGI321| + TP3) 0.0722 HIF411 1.5056 HIF411/HOI 0.4562 SGI411 0.4677 |SGI411|/(|SGI411| + TP4) 0.5366 HIF412 2.4486 HIF412/HOI 0.7420 SGI412 0.8386 |SGI412|/(|SGI412| + TP4) 0.6749 HIF421 1.9207 HIF421/HOI 0.5820 SGI421 0.6588 |SGI421|/(|SGI421| + TP4) 0.6200 HIF422 2.7963 HIF422/HOI 0.8474 SGI422 1.0419 |SGI422|/(|SGI422| + TP4) 0.7207 HIF511 2.1788 HIF511/HOI 0.6603 SGI511 1.0304 |SGI511|/(|SGI511| + TP5) 0.5648 HIF521 2.0340 HIF521/HOI 0.6164 SGI521 0.8280 |SGI521|/(|SGI521| + TP5) 0.5105 HIF611 1.0243 HIF611/HOI 0.3104 SGI611 −0.0265 |SGI611|/(|SGI611| + TP6) 0.0235 HIF612 2.2118 HIF612/HOI 0.6702 SGI612 0.0111 |SGI612|/(|SGI612| + TP6) 0.0099 HIF621 1.4424 HIF621/HOI 0.4371 SGI621 −0.3745 |SGI621|/(|SGI621| + TP6) 0.2534 HIF622 2.4861 HIF622/HOI 0.7534 SGI622 −0.5198 |SGI622|/(|SGI622| + TP6) 0.3202 HIF711 0.6244 HIF711/HOI 0.1892 SGI711 0.0309 |SGI711|/(|SGI711| + TP7) 0.0586 HIF712 2.1949 HIF712/HOI 0.6651 SGI712 −0.0179 |SGI712|/(|SGI712| + TP7) 0.0349 HIF713 2.9170 HIF713/HOI 0.8839 SGI713 −0.0366 |SGI713|/(|SGI713| + TP7) 0.0688 HIF721 0.8213 HIF721/HOI 0.2489 SGI721 0.1633 |SGI721|/(|SGI721| + TP7) 0.2477 HIF722 2.9374 HIF722/HOI 0.8901 SGI722 0.2348 |SGI722|/(|SGI722| + TP7) 0.3213

It must be pointed out that the embodiments described above are only some embodiments of the present invention. All equivalent structures which employ the concepts disclosed in this specification and the appended claims should fall within the scope of the present invention. 

What is claimed is:
 1. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane specifically for infrared light; wherein the optical image capturing system has a total of the seven lenses with refractive power; at least one lens among the first lens to the seventh lens has positive refractive power; each lens among the first lens to the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 0.5≤f/HEP≤1.8; 0 deg<HAF≤50 deg; and 0.9≤2(ARE/HXP)≤2.0; wherein f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HXP is an exit pupil diameter of the image-side surface of the seventh lens; HAF is a half of a maximum field angle of the optical image capturing system; for any surface of any lens, ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the exit pupil diameter away from the optical axis.
 2. The optical image capturing system of claim 1, wherein a wavelength of the infrared light ranges from 700 nm to 1300 nm, and a first spatial frequency is denoted by SP1, which satisfies the following condition: SP1≤440 cycles/mm.
 3. The optical image capturing system of claim 1, wherein a wavelength of the infrared light ranges from 850 nm to 960 nm, and a first spatial frequency is denoted by SP1, which satisfies the following condition: SP1≤220 cycles/mm.
 4. The optical image capturing system of claim 3, wherein the optical image capturing system further satisfies: PLTA≤100 μm; PSTA≤100 μm; NLTA≤100 μm; NSTA≤100 μm; SLTA≤100 μm; SSTA≤100 μm; and |TDT|≤100%; wherein TDT is a TV distortion; HOI is a maximum height for image formation on the image plane specifically for infrared light perpendicular to the optical axis; PLTA is a transverse aberration at 0.7 HOI on the image plane specifically for infrared light in the positive direction of a tangential fan of the optical image capturing system after a longest operation wavelength of infrared light passing through an edge of the aperture, wherein the longest operation wavelength is 960 mm; PSTA is a transverse aberration at 0.7 HOI on the image plane specifically for infrared light in the positive direction of the tangential fan after a shortest operation wavelength of infrared light passing through the edge of the aperture, wherein the shortest operation wavelength is 850 nm; NLTA is a transverse aberration at 0.7 HOI on the image plane specifically for infrared light in the negative direction of the tangential fan after the longest operation wavelength of infrared light passing through the edge of the aperture; NSTA is a transverse aberration at 0.7 HOI on the image plane specifically for infrared light in the negative direction of the tangential fan after the shortest operation wavelength of infrared light passing through the edge of the aperture; SLTA is a transverse aberration at 0.7 HOI on the image plane specifically for infrared light of a sagittal fan of the optical image capturing system after the longest operation wavelength of infrared light passing through the edge of the aperture; SSTA is a transverse aberration at 0.7 HOI on the image plane specifically for infrared light of a sagittal fan after the shortest operation wavelength of infrared light passing through the edge of the aperture.
 5. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.9≤ARS/EHD≤2.0; wherein, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 6. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: IN56>IN23; wherein IN23 is a distance on the optical axis between the second lens and the third lens, and IN56 is a distance on the optical axis between the fifth lens and the sixth lens.
 7. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: IN56>IN34; wherein IN34 is a distance on the optical axis between the third lens and the fourth lens, and IN56 is a distance on the optical axis between the fifth lens and the sixth lens.
 8. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: IN56>IN45; wherein IN45 is a distance on the optical axis between the fourth lens and the fifth lens, and IN56 is a distance on the optical axis between the fifth lens and the sixth lens.
 9. The optical image capturing system of claim 1, further comprising an aperture, wherein the optical image capturing system further satisfies: 0.2≤InS/HOS≤1.1; wherein InS is a distance between the aperture and the image plane specifically for infrared light on the optical axis, and HOS is a distance between the object-side surface of the first lens and the image plane specifically for infrared light on the optical axis.
 10. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane specifically for infrared light; wherein the optical image capturing system has a total of the seven lenses with refractive power; at least one surface of at least one lens among the first lens to the seventh lens has at least an inflection point thereon; at least one lens among the first lens to the seventh lens has positive refractive power; each lens among the first lens to the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 9.5≤f/HEP≤1.5; 0 deg<HAF≤50 deg; and 0.9≤2(ARE/HXP)≤2.0; wherein f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HXP is an exit pupil diameter of the image-side surface of the seventh lens; HAF is a half of a maximum field angle of the optical image capturing system; for any surface of any lens, ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the exit pupil diameter away from the optical axis.
 11. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0.9≤ARS/EHD≤2.0; wherein, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 12. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0.5≤HOS/HOI≤4; wherein HOS is a distance between the object-side surface of the first lens and the image plane specifically for infrared light on the optical axis; HOI is a maximum height for image formation on the image plane specifically for infrared light perpendicular to the optical axis.
 13. The optical image capturing system of claim 10, further comprising an aperture disposed before the image-side surface of the third lens.
 14. The optical image capturing system of claim 10, wherein the image-side surface of the first lens is concave on the optical axis.
 15. The optical image capturing system of claim 10, wherein the object-side surface of the second lens is convex on the optical axis.
 16. The optical image capturing system of claim 10, wherein the object-side surface of the fourth lens is convex on the optical axis, and the image-side surface of the fourth lens is concave on the optical axis.
 17. The optical image capturing system of claim 10, wherein the object-side surface of the fifth lens is convex on the optical axis, and the image-side surface of the fifth lens is concave on the optical axis.
 18. The optical image capturing system of claim 10, wherein at least one lens among the first lens to the seventh lens is made of plastic.
 19. The optical image capturing system of claim 10, wherein the first lens to the seventh lens are all made of plastic.
 20. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane specifically for infrared light; wherein the optical image capturing system has a total of the seven lenses having refractive power; at least one surface of each of at least two lenses among the first lens to the seventh lens has at least an inflection point thereon; each lens among the first lens to the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 0.5≤f/HEP≤1.4; 0 deg<HAF≤45 deg; and 0.9≤2(ARE/HXP)≤2.0; wherein f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HXP is an exit pupil diameter of the image-side surface of the seventh lens; HAF is a half of a maximum field angle of the optical image capturing system; for any surface of any lens, ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the exit pupil diameter away from the optical axis.
 21. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 0 mm<HOS≤20 mm; wherein HOS is a distance between the object-side surface of the first lens and the image plane specifically for infrared light on the optical axis.
 22. The optical image capturing system of claim 20, wherein a wavelength of the infrared light ranges from 850 nm to 960 nm, and a first spatial frequency is denoted by SP1, which satisfies the following condition: SP1≤220 cycles/mm.
 23. The optical image capturing system of claim 20, wherein the first lens to the seventh lens are all made of plastic.
 24. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: IN56>IN23; IN56>IN34; and IN56>IN45; wherein IN23 is a distance on the optical axis between the second lens and the third lens, IN34 is a distance on the optical axis between the third lens and the fourth lens, IN45 is a distance on the optical axis between the fourth lens and the fifth lens, and IN56 is a distance on the optical axis between the fifth lens and the sixth lens.
 25. The optical image capturing system of claim 20, further comprising an aperture and an image sensor, wherein the optical image capturing system further satisfies: 0.2≤InS/HOS≤1.1; wherein the image sensor is disposed on the image plane specifically for infrared light and is provided with at least one hundred thousand pixels, and InS is a distance between the aperture and the image plane specifically for infrared light on the optical axis; HOS is a distance between the object-side surface of the first lens and the image plane specifically for infrared light on the optical axis. 